WO2012083585A1 - Well logging device, well logging method and data processing apparatus - Google Patents

Well logging device, well logging method and data processing apparatus Download PDF

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Publication number
WO2012083585A1
WO2012083585A1 PCT/CN2011/002099 CN2011002099W WO2012083585A1 WO 2012083585 A1 WO2012083585 A1 WO 2012083585A1 CN 2011002099 W CN2011002099 W CN 2011002099W WO 2012083585 A1 WO2012083585 A1 WO 2012083585A1
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WO
WIPO (PCT)
Prior art keywords
phase difference
formation
amplitude ratio
logging
measurement point
Prior art date
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PCT/CN2011/002099
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French (fr)
Chinese (zh)
Inventor
杨锦舟
李作会
林楠
魏宝君
刘庆龙
肖红兵
Original Assignee
中国石油化工股份有限公司
中国石化集团胜利石油管理局钻井工艺研究院
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
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Application filed by 中国石油化工股份有限公司, 中国石化集团胜利石油管理局钻井工艺研究院 filed Critical 中国石油化工股份有限公司
Priority to GB1311636.3A priority Critical patent/GB2500156B/en
Priority to US13/996,149 priority patent/US9377555B2/en
Priority to NO20131015A priority patent/NO346394B1/en
Priority to CA2822506A priority patent/CA2822506C/en
Priority to JP2013545012A priority patent/JP5944923B2/en
Publication of WO2012083585A1 publication Critical patent/WO2012083585A1/en
Priority to US15/167,490 priority patent/US9927548B2/en

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/08Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation operating with magnetic or electric fields produced or modified by objects or geological structures or by detecting devices
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/18Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging
    • G01V3/26Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging operating with magnetic or electric fields produced or modified either by the surrounding earth formation or by the detecting device
    • G01V3/28Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging operating with magnetic or electric fields produced or modified either by the surrounding earth formation or by the detecting device using induction coils
    • EFIXED CONSTRUCTIONS
    • E21EARTH DRILLING; MINING
    • E21BEARTH DRILLING, e.g. DEEP DRILLING; OBTAINING OIL, GAS, WATER, SOLUBLE OR MELTABLE MATERIALS OR A SLURRY OF MINERALS FROM WELLS
    • E21B49/00Testing the nature of borehole walls; Formation testing; Methods or apparatus for obtaining samples of soil or well fluids, specially adapted to earth drilling or wells
    • EFIXED CONSTRUCTIONS
    • E21EARTH DRILLING; MINING
    • E21BEARTH DRILLING, e.g. DEEP DRILLING; OBTAINING OIL, GAS, WATER, SOLUBLE OR MELTABLE MATERIALS OR A SLURRY OF MINERALS FROM WELLS
    • E21B7/00Special methods or apparatus for drilling
    • E21B7/04Directional drilling
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/18Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging
    • G01V3/30Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging operating with electromagnetic waves

Definitions

  • the present invention relates to the field of logging technology, and more particularly, the present invention relates to the field of drilling while drilling technology, and in particular, the invention relates to a logging device, a logging method and a corresponding method for geosteering in a drilling engineering. Data processing equipment. Background technique
  • formation resistivity is often used to form stratigraphic profiles and determine reservoir oil saturation. Degree, gas content of coal structure and mineral faults, so formation resistivity is the main basis for logging interpretation and evaluation of oil and gas, coal and mineral storage.
  • Known drilling-while-drilling resistivity logging techniques include LWD lateral resistivity logging, LWD electromagnetic transmission resistivity logging, and LWD induction resistivity logging.
  • the working principle of the lateral resistivity logging device while drilling is mainly to provide current by the power supply electrode, form an electric field in the formation around the wellbore, measure the distribution of the electric field in the formation, and obtain the formation resistivity.
  • the while-drilling lateral resistivity logging device uses the drill bit itself as an electrode. It is also possible to use a ring electrode and three button electrodes close to the drill bit for resistivity measurement. With the drill bit as the electrode, the LWD lateral resistivity logging device can measure the resistivity of a 5-10 cm thin layer before the mud intrusion or the wellbore may be damaged.
  • the LWD lateral logging resisting device has the following disadvantages: Because the lateral resistivity logging is a DC logging, the first step is to have a supply electrode to direct the DC current into the formation, and then use a measuring electrode to measure a point in the well. The potential, so this lateral resistivity logging method can only be used when there is conductive mud in the well to provide a current path. However, during actual drilling operations, such as during oil drilling, sometimes oil-based mud drilling is required to obtain the original oil saturation information of the formation, even using air drilling. Under such conditions, direct current measurement cannot be used. Wells, ie, while drilling lateral resistivity logging methods, are no longer applicable in these situations.
  • the electromagnetic wave propagation resistivity logging device while drilling uses a multi-wire tether design with a propagation frequency of 1 ⁇ 8MHz, the coil is based on the body structure of the drill collar, and the coil system is wound on the drill collar.
  • the phase shift is measured shallow.
  • Resistivity and attenuation of deep resistivity are measured shallow.
  • the longitudinal resolution of the electromagnetic wave propagation resistivity logging device is determined by the spacing of the two receiving coils.
  • the measurement data of the multiple detection depths can be used to explain the intrusion condition. It is generally considered that the phase resistivity is shallow.
  • the decay resistivity has a large depth of detection.
  • the publication entitled CN101609169A entitled “A Method for Improving the Measurement Accuracy of Electromagnetic Wave Resistivity and Extending the Measurement Range” discloses the calculation of the mutual inductance electromotive force between the transmitting antenna and the receiving antenna, eliminating the amplitude attenuation of the mutual inductance electromotive force.
  • a resistivity conversion diagram and a phase difference-resistivity conversion diagram are the mutual inductance electromotive force, the circuit zero signal, and the antenna system base value signal independent of the formation resistivity, and the phase difference and the amplitude attenuation are converted to the formation resistivity.
  • the measurement results of the electromagnetic wave propagation resistivity logging device while drilling will be affected by geological factors, especially the surrounding rock, because the measurement results of the device are not limited to the formation area between the receiving coils, and the transmitting coil to the receiving
  • the entire formation parameter between the turns is related, even the formation in a smaller area around the launch line will have an impact on the measurement results, so the vertical resolution of the logging device depends to a large extent on the entire device.
  • the resistivity of the formation is not limited to the formation area between the receiving coils, and the transmitting coil to the receiving
  • the manufacturing process is very complicated, and the coil system is extremely susceptible to wear and damage during use, and when the well is drilled When the size changes, the coil needs to be re-rolled, and the maintenance inspection is complicated and the maintenance cost is high.
  • the electromagnetic wave propagation resistivity logging device cannot be operated in oil-based mud.
  • the on-board induction resistivity logging device utilizes the principle of electromagnetic induction.
  • an eddy current When an alternating current of constant amplitude and frequency is applied to the emission line, an eddy current is induced in the surrounding formation of the coil, and the eddy current itself forms a secondary alternating electromagnetic field. Under the action of the secondary alternating electromagnetic field, an induced electromotive force is generated in the receiving coil. The magnitude of the electromotive force is related to the conductivity of the formation. The formation resistivity can be obtained by measuring the induced electromotive force.
  • the coil of the induction-resistance resistivity logging device adopts one transmitting coil and two receiving coils, one of the two receiving coils is a main receiving coil, and the other is a compensating coil, and the coil is placed on the drill.
  • the logging response is sensitive to the resistivity change of the formation in the front area of the V-shaped groove, and therefore has the characteristics of directional measurement.
  • the while-drilling resistivity logging device is powered by a battery, and a male snap connector is attached to the top of the battery.
  • the male snap connector can be connected to the female snap connector at the bottom of the LWD logging device for
  • the LWD inductive resistivity logging device delivers real-time data, and the same sensor sub-section can be used for different sizes of wellbore requirements.
  • the advantages of this MWD logging device are:
  • the signal frequency is 20 kHz, which is much lower than the frequency of the high frequency device, so it is not easily absorbed by the formation.
  • the depth of detection is deep and the measurement range is large, which can reach 0.1-1000 ohms.
  • M and its structural design is simple, a sensor sub-section can be applied to the needs of different sizes of wells, maintenance inspection is simple, and different types of drilling fluids are applicable.
  • Drilling Induction Resistivity Logging Device has the following disadvantages: Since the device employs a coil system consisting of one transmitting coil and two receiving turns with a single fixed depth of detection, the logging device can only Providing a formation resistivity with a radial depth of investigation cannot be used to explain complex intrusion profiles and to divide the permeable layer. In addition, for the permeable layer, the mud intrusion causes the resistivity to change radially. Since only one radial detection depth resistivity value can be obtained at the same depth point, the LWD induction logging device cannot be used.
  • the present invention provides a new logging while drilling method, which can not only measure the forward resistivity change of the well in real time during the drilling process, but also distinguish different resistivity layers in front of the drilling process. Interface features.
  • a logging method comprising:
  • a data processing device characterized in that the data processing device comprises:
  • the homogeneous formation optional point determining device (1403, 1404) is used for determining whether two consecutive measuring points currently selected by the logging device can be used as the selective points of the homogeneous formation;
  • a base value determining device for determining, based on the two selectable points of the homogeneous formation layer, if the determination result of the homogeneous formation point selectable device (1403, 1404) is YES
  • the amplitude of the induced signal of the logging device corresponding to the formation resistivity of the measured high resistance target layer is greater than the base value and the phase difference base value;
  • a standard value determining device for determining an amplitude ratio standard value and a phase difference standard value corresponding to a formation resistivity of the measured high resistance target layer according to the amplitude ratio base value and the phase difference base value;
  • a layer threshold setting device (1408) configured to set an exit threshold of the measured high resistance target layer according to the amplitude ratio standard value and a phase difference standard value;
  • a third-th nth measuring point selection and calculating device for continuously selecting the next measuring point for at least two measurements, and calculating a pair of receiving coils of the logging device at the currently selected measuring point The magnitude of the induced electromotive force between the amount of change and the amount of change in phase difference;
  • a low-resistance formation determining device comprising an out-of-layer threshold determining unit (14101), configured to determine whether an amplitude ratio change amount and/or a phase difference change amount at the currently selected measurement point is greater than The exit threshold; if so, it is determined that a low-resistance formation is present in front of the logging device.
  • a logging apparatus characterized in that the logging apparatus comprises a drill collar body (12) and an antenna array, wherein the antenna array comprises at least one pair of transmitting antennas and receiving antennas, The transmit and receive antennas are used to generate a forward detected depth profile.
  • the forward depth detection according to the present invention has the following important significance: First, the forward depth detection according to the present invention can effectively control the trajectory of the drilling engineering slant section; the well-known horizontal section measurement formation usually The horizontal layered distribution is assumed first. When the slanting is started, the resistivity logging device is nearly perpendicular to the horizontal layered strata, so the radial detection response can only reflect the change of the resistivity of the measured formation at a certain level.
  • the response to the probe has multiple forward detection depths, which reflect the change in resistivity of the measured formation at different depths of the well, which can effectively identify the layer boundary and the oil-water contact, and adjust the oblique curvature.
  • the forward depth detection according to the present invention can perform forward detection of different depths on the front end of the drilling well, which is more direct and accurate than the radial detection method. Pre-determine thin oil layers, complex folds and mutual interlayers, so as to effectively bypass the faults and drill long distances along the high dip reservoir to obtain the highest oil and gas effective drilling rate.
  • the logging method and the corresponding data processing device can measure the change characteristics of the resistivity change rate of the formation in real time during the drilling process, and accurately resolve the formation interface and the oil-water interface in real time, and capture the optimal timing of entering the oil and gas reservoir.
  • the geological information in front of the drill bit can be predicted for a long distance and the well trajectory can be adjusted in time to control the drilling tool to travel through the optimal position of the reservoir, so as to obtain the maximum oil-touch surface, which is very suitable for Geosteering in petroleum engineering.
  • Figure 1 shows a logging device in accordance with a preferred embodiment of the present invention
  • Figure 2 is a diagram showing a two-layer formation model used in the logging method according to the present invention
  • Figure 3 is a graph showing the relationship between the amplitude attenuation response of the formation and the position of the formation interface with a resistivity contrast of 10/1;
  • Figure 4 shows the relationship between the displacement response of the formation with the resistivity contrast of 10/1 and the position of the formation interface
  • Figure 5 shows the relationship between the amplitude attenuation response of the formation with a resistivity contrast of 50/1 and the position of the formation interface
  • Figure 6 shows the relationship between the displacement response of the formation with the resistivity contrast of 50/1 and the position of the formation interface
  • Figure 7 is a graph showing the relationship between the amplitude attenuation response of the formation and the position of the formation interface with a resistivity contrast of 200/1;
  • Figure 8 is a graph showing the relationship between the displacement response of the formation and the position of the formation interface with the resistivity contrast of 200/1;
  • FIG. 9 is a comparison table of various measured formation resistivity and amplitude ratios and phase difference eigenvalues of the antenna system T2-R1 - R2 in the logging device according to a preferred embodiment of the present invention at a transmission frequency of 2 MHz. ;
  • Figure 10 illustrates various measured formation resistivity and amplitude ratios of antenna systems T2-R1 - R2 in a logging device in accordance with a preferred embodiment of the present invention at an emission frequency of 400 kHz. a comparison table of eigenvalues of phase differences;
  • Figure 1 1 shows a comparison of various measured formation resistivity versus amplitude ratios and eigenvalues of phase differences for antenna systems T1 - R1 - R2 in a logging device in accordance with a preferred embodiment of the present invention at a transmission frequency of 2 MHz.
  • Figure 12 is a table showing the measured values of formation resistivity versus amplitude ratio and phase difference of the antenna system T1 - R1 - R2 in the logging device in accordance with a preferred embodiment of the present invention at an emission frequency of 400 kHz. ; detailed description:
  • Coupled coupling includes Direct coupling and indirect coupling via additional components, components, circuits, or modules, where indirect coupling, components, components, circuits, or modules do not alter signal information but can adjust their current levels, voltages Horizontal, and/or power levels.
  • Inferred coupling eg, one element is inferred to another element by inference
  • FIG. 1 shows a logging device, an electromagnetic wave propagation resistivity detecting device, comprising a drill collar body 12, an antenna array 7-1 1 , 13-15, an internal electronic circuit (in the figure) according to a preferred embodiment of the present invention. Not shown) and a cured seal for coupling the components.
  • the drill collar body 12 is preferably made of a stainless steel material having a cylindrical shape and an axial through hole in the present embodiment, and the outer surface of the drill collar body 12 is preferably engraved with a large amount.
  • a ring or an elliptical groove is used to mount the transmitting or receiving antenna.
  • the antenna array comprises four transmit antennas T1 (as indicated by reference numeral 1), T2 (as indicated by reference numeral 14), and T3 (as indicated by reference numeral 13). Show) and T4 (as indicated by reference numeral 15), and 4 receiving antennas R1 (as indicated by reference numeral 7), R2 (as indicated by reference numeral 8), R3 (as indicated by reference numeral 9) ) and R4 (as indicated by reference numeral 10).
  • the order of arrangement of the transmitting antenna and the receiving antenna from the left side of FIG. 1 to the right side of FIG. 1 is preferably: receiving antenna R3, A transmitting antenna T3, a transmitting antenna T1, a receiving antenna R1, a receiving antenna R2, a transmitting antenna T2, a transmitting antenna ⁇ 4, and a receiving antenna R4.
  • the midpoint between the receiving antennas R1 and R2 is a measuring point
  • the transmitting antennas T1, ⁇ 2, ⁇ 3 and ⁇ 4 are preferably symmetrically mounted around the measuring point, respectively.
  • the receiving antennas R1 and R2 are preferably receiving antenna pairs with a mounting angle of zero, and the receiving antennas R3 and R4 are another pair of receiving antennas with the measuring point as a center of symmetry, as shown in FIG. R3 and R4 are preferably located at both ends of the drill collar.
  • the mounting angles of the receiving antennas R3 and R4 can be arbitrarily set, and in the present embodiment, they are preferably, but not limited to, set to 45° and -45°.
  • the electromagnetic signal propagates through the surrounding ground and the drill collar body, and is reflected and transmitted through the ground layer.
  • An electromagnetic induction signal is generated on the receiving antenna, and the electromagnetic induction signal is collected by the receiving antenna, then subjected to signal processing such as amplification and filtering via the internal electronic circuit, and finally converted into a function of the resistivity of the propagating formation.
  • the logging device in this embodiment, the electromagnetic wave propagation resistivity detecting device
  • the formation electrical parameters such as formation resistivity contrast
  • the electricity reflected to the receiving antenna at this time The magnetic signal will not change, and if the electrical parameters of the formation in front of the device change, it means that a layer boundary appears, and the electromagnetic signal reflected to the receiving antenna will change, resulting in a signal difference, constantly This signal difference is calculated and calculated, and the distance of forward detection can be obtained.
  • a combination of any of the transmitting antennas and any of the sets of receiving antennas in the logging device can generate a forward detecting curve through all of the front Comparing and processing the detection curve can eliminate environmental influences (such as wellbore effects) and measurement errors, thereby improving the forward detection accuracy of the logging device.
  • a logging method according to a preferred embodiment of the present invention - a method for forward detection of electromagnetic wave resistivity includes the following steps:
  • a logging while drilling device (preferably, for example, an electromagnetic wave propagation resistivity forward detecting device shown in FIG. 1) is placed in a high resistance target layer at a certain depth position, while the logging device continues to drill.
  • the logging device performs continuous detection with a direction of detection that coincides with the direction of axial movement of the logging device (preferably the electromagnetic wave propagation resistivity forward detecting device shown in the figure).
  • step 1302 two consecutive measurement points (e.g., a first measurement point and a second measurement point) are selected, and at least two consecutive measurements are taken at each measurement point.
  • two consecutive measurement points e.g., a first measurement point and a second measurement point
  • step 1303 if the amplitude ratio of the induced electromotive force between the first receiving line and the second receiving line in the axial direction of the logging device in the at least two consecutive measurements at the first measuring point is changed
  • the quantity ⁇ " and the phase difference change amount A PSD are in their respective predetermined threshold ranges (for example, the predetermined amplitude ratio variation amount threshold value may be 0-0.03 dB or other predetermined range, and the predetermined phase difference variation amount threshold value range is 0° Within -0. 1° or other predetermined range)
  • the first measurement point is saved as a select point of the first homogeneous formation.
  • step 1304 if the amplitude ratio of the induced electromotive force between the first receiving line and the second receiving line in the axial direction of the logging device in the at least two consecutive measurements at the second measuring point is changed
  • the quantity ⁇ 1 " and the phase difference variation A PSD are both within the respective predetermined threshold ranges, and the second measurement point is saved as a second homogeneous formation optional point.
  • steps 1303 and 1304 If it is determined in steps 1303 and 1304 that two homogeneous formation selectable points satisfying the above conditions are not found, then return to step 1302 to continue the measurement while drilling, and so on. Until you find a selection of two homogeneous formations that meet the criteria.
  • the first received line measured at the first and second homogeneous formation optional points An average of amplitude ratios of induced electromotive forces between the ⁇ and the second receiving line ( (ie, an average of a plurality of amplitude ratios obtained for each measurement performed at the selectable points of the two homogeneous formations) or The average of the root mean square and phase difference (the average of multiple phase differences obtained from each measurement at two selectable points in the homogeneous formation) or the root mean square as the formation of the layer with the measured high resistance
  • the magnitude of the induced signal of the logging device corresponding to the resistivity is greater than the base value "0" and the phase difference base value PSDQ.
  • step 1306 the standard value of the formation resistivity of the measured high resistance target layer is determined and stored, that is, the above amplitude ratio base value corresponding to the formation resistivity of the measured high resistance target layer is ⁇ 0.
  • the phase difference base value ⁇ 3 ⁇ 4) ⁇ is compared with the corresponding predetermined eigenvalues of the various formations, and the type of ground and phase difference standard values closest to the base value and the phase difference base value are selected and stored. The amplitude is greater than the standard value and the phase difference standard value.
  • the exit threshold of the measured high resistance target layer is set according to an amplitude ratio standard value and a phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer. Specifically, when the logging device is close to the low resistance boundary, the amplitude ratio and the phase difference of the induced electromotive force between the first receiving coil and the second receiving coil in the axial direction of the logging device are caused.
  • the measured amplitude ratio is the variation (ie, the difference) with respect to the standard value of the amplitude ratio, and the variation of the measured phase difference with respect to the standard value of the phase difference (ie, The larger the difference), when the amplitude ratio change and the phase difference change amount reach or exceed a predetermined value, it is generally considered that a low-resistance formation appears in front of the logging device.
  • the predetermined value is the exit threshold as described herein. It should be noted that the ejecting threshold can be set to different predetermined values according to the characteristics and measurement conditions of the actual measured stratum for the different measured strata by the person skilled in the art, generally through the current measured stratum and the front stratum.
  • the resistivity contrast is determined.
  • the exit threshold can be set to an amplitude ratio of 1% of the standard value or the phase difference standard value regardless of the resistivity contrast of the two layers of the current measured formation and the front formation. 30%; Further preferably, when the resistivity contrast is 1 /10, the layer threshold may preferably be set to 10% of the amplitude ratio standard value or phase difference standard value.
  • the manner of determining the above-mentioned layering threshold and the numerical values are merely exemplary, and should not constitute a limitation on the scope of the present invention.
  • the next measurement point is continued, at least two measurements are taken at the next measurement point, and the first receive coil and the second along the axial direction of the logging device at the measurement point are calculated.
  • step 1309 it is determined whether the amplitude ratio change amount ⁇ " and the phase difference change amount A PSD calculated in step 1308 are greater than the exit threshold; if greater, it is determined that the front of the logging device is a low-resistance formation; If not greater than, the current amplitude ratio change amount "and the phase difference change amount A PSD is stored, and then it is determined whether the predetermined nth measurement point has been reached. If not, then return to step 1308 to continue the selection and amplitude of the next measurement point. The calculation of the ratio change amount and the phase difference change amount A PSD , if it is the predetermined nth measurement point, proceeds to step 1310.
  • the ⁇ is selected by the technician according to the actual situation according to the characteristics of the formation and the measured speed. For example, if it is for a softer stratum (such as sandstone in the Bohai area), the value of ⁇ It can be relatively small, and for harder formations (such as shale), the value of ⁇ can be relatively large. Generally, for ordinary formations, ⁇ is preferably 20-30, but the invention is absolutely Without being limited thereto, it may be other suitable values.
  • the overall same-directional increase described herein means: although there is an ups and downs in the middle of the change trend (ie It is said that the amplitude ratio change amount and the phase difference change amount at a certain measurement point are reduced with respect to the amplitude ratio change amount and the phase difference change amount at the previous measurement point), but for example, at least 70% of the measurement points
  • the trend of increasing in the same direction is maintained, and the percentage is also preset by the technician according to the actual measurement situation.
  • the 70% is merely exemplary and does not constitute a limitation on the scope of protection of the present invention.
  • the formation of the first and second homogeneous layer selectable points may be calculated by the magnetic dipole source dyadic Green's function. Resistivity, amplitude ratio, and phase difference.
  • Figures 9-12 illustrate several exemplary eigenvalue comparison tables for measuring formation resistivity versus amplitude ratio and phase difference, the corresponding physical quantities in the eigenvalue comparison table passing through the magnetic dipole source and The vector green function is calculated.
  • FIG. 9 is a comparison of various measured formation resistivity and amplitude ratios and phase difference converted eigenvalues of the logging device antenna for T2-R1 -R2 at a transmission frequency of 2 MHz according to a preferred embodiment of the present invention.
  • Figure 10 shows a comparison of various measured formation resistivity and amplitude ratios and phase difference converted eigenvalues of a logging device antenna for T2-R1 - R2 at a transmission frequency of 400 kHz in accordance with a preferred embodiment of the present invention.
  • Figure 1 1 shows various measured formation resistivity and amplitude ratios and phase difference converted eigenvalues of a logging device antenna for T 1 -R1 -R2 at a transmission frequency of 2 MHz in accordance with a preferred embodiment of the present invention.
  • Figure 12 shows the eigenvalues of various measured formation resistivity and amplitude ratios and phase difference conversions of the logging device antenna for T1 - R1 - R2 at a transmission frequency of 400 kHz in accordance with a preferred embodiment of the present invention. Comparison table.
  • the logging method preferably further comprises calculating a front low resistance formation to a logging device using a Sommerfeld integral (eg, an electromagnetic wave propagation resistivity forward detecting device in accordance with the present invention) the distance.
  • a Sommerfeld integral eg, an electromagnetic wave propagation resistivity forward detecting device in accordance with the present invention
  • Figure 2 of the present application shows a two-layer formation model diagram preferably used in a logging method for forward detection of an electromagnetic wave propagation resistivity forward detecting device in accordance with a preferred embodiment of the present invention.
  • each reference numeral denotes: formation 1; 2: formation 2; 3: layer interface between formation 1 and formation 2; 4: electromagnetic wave propagation resistivity forward detection device core axis; 5: Electromagnetic wave propagation resistivity measurement point of the forward detecting device; 6: Electromagnetic wave propagation resistivity The distance from the measuring point of the forward detecting device to the layer interface 3 between the ground layer 1 and the ground layer 2; 7: The receiving antenna R1 with a mounting angle of zero; 8: receiving antenna R2 with a mounting angle of preferably zero degrees; 9: receiving antenna R3 with a mounting angle of preferably 45°; 10: receiving antenna R4 with a mounting angle of preferably -45°; 1 1 , a transmitting antenna with a mounting angle of preferably zero Tl.
  • the electromagnetic wave propagation resistivity forward detecting device is disposed in the formation 1 and perpendicular to the interface of the formation 1 and the formation 2, and can be obtained by changing the distance between the formation interface 3 and the center point of the device.
  • 3 to 8 illustrate amplitude attenuation responses or phase shifts of different transmit-receive antenna pairs in different resistivity contrast formations when different frequencies are employed, in accordance with a preferred embodiment of the present invention. Respond to changes in the position of the interface with the ground plane.
  • the amplitude-attenuation threshold of the electromagnetic wave propagation resistivity forward detecting device is 0.02 dB, and the phase shift threshold is 0. ⁇ (shown by the horizontal line in FIGS. 3-8) 3 to 8 can obtain the vertical depth of detection of each pair of antennas in the detection device in different resistivity contrast formations.
  • the amplitude attenuation of the 16/22 in. (ie inches) antenna pair and the vertical depth of the phase shift are 41 in. And 26 in., 32/38 ⁇ .
  • the amplitude attenuation of the antenna pair and the vertical depth of the phase shift are 56 in. and 37 in. respectively; if the frequency of the transmit-receive antenna pair is 400 kHz, the 16/22 in. antenna pair
  • the amplitudes of the amplitude attenuation and phase shift are 43 in. and 35 in., respectively, and the 32/38 in. antenna pair amplitude attenuation and phase displacement vertical detection depth are 67 in. and 48 in., respectively.
  • the amplitude attenuation of the 16/22in. antenna pair and the vertical depth of the phase shift are 55 in. and 35 in., 32/38 in.
  • the vertical attenuation depths of the amplitude attenuation and phase shift are 77 in. and 46 in. respectively; if the frequency is 400 kHz, the amplitude attenuation of the antenna pair and the vertical displacement of the phase shift ⁇ !
  • the amplitudes of amplitude attenuation and phase shift of the antenna pairs of 49 in. and 44 in., 32/38 in. respectively are 82 in. and 62 ⁇ .
  • the amplitude attenuation of the 16/22 in. antenna pair and the vertical depth of phase shift are 61 in. and 43 in., 32/38 in. antenna, respectively.
  • the vertical depths of amplitude attenuation and phase shift are 92 in. and 57 in. respectively; if the frequency is 400 kHz, the amplitude attenuation of the 16/22 in. antenna pair and the vertical depth of phase shift are 50 respectively. In. and 47 in. , 32/38 in.
  • the amplitude attenuation of the antenna pair and the vertical depth of phase shift are 87 in. and 71 in., respectively.
  • the presence of the formation interface or the oil-water interface may be determined by measuring the amplitude attenuation or the phase shift signal in real time by the logging while drilling device disposed in the drilling device according to the present invention during the forward drilling of the drilling device. This controls the drill to travel through the best position in the reservoir. If the LWD tool does not exhibit the above-mentioned amplitude attenuation or phase shift signal change during the drilling of the drilling device, that is, the amplitude attenuation of the LWD device or the reading of the phase shift signal is constant. This means that there is no low-resistance formation.
  • the drilling unit is always located in the high-resistance oil-bearing purpose interval, thereby achieving pre-drilling prediction and precise geosteering of the formation interface.
  • the logging apparatus and logging method of the present invention are not limited to the field of oil drilling, but are also widely applicable to other drilling industries such as coal mining and mining. .
  • the data processing apparatus preferably includes: first and second measurement point selecting means 1400, first amplitude ratio change amount and phase difference change amount calculating means 1401, second amplitude ratio change amount and Phase difference variation calculation device 1402, first homogeneous formation optional point determination device 1403, second homogeneous formation optional point determination device 1404, storage device 1405, base value determination device 1406, standard value determination device 1407, and egress layer Threshold setting means 1408, third-nth measurement point selection and calculation means 1409 and low resistance formation determination means 1410.
  • the first and second measurement point selection devices 1400 select two consecutive measurement points (ie, a first measurement point and a second measurement point), and instruct the logging device to perform at least two at each selected measurement point. Sub-continuous measurement.
  • the first and second measurement point selecting means 1400 are coupled to the first amplitude ratio change amount and phase difference change amount calculating means 1401 and the second amplitude ratio change amount and phase difference change amount calculating means 1402, respectively.
  • the first amplitude ratio change amount and phase difference change amount calculation means 1401 is configured to calculate at the first measurement point selected by the first and second measurement point selection means 1400, An amplitude ratio change amount A ⁇ t and a phase difference change amount A PSD of the induced electromotive force between the first receiving coil and the second receiving coil in the axial direction of the logging device in at least two consecutive measurements; the second amplitude ratio The variation and phase difference variation calculation device 1402 is configured to calculate the axial direction along the logging device at the second measurement point selected by the first and second measurement point selection devices 1400 in the at least two consecutive measurements An amplitude ratio change amount ⁇ " of the induced electromotive force between the first receiving line ⁇ and the second receiving line ⁇ and a phase difference change amount A PSD; the first homogeneous formation selectable point determining device 1403 is coupled to the The first amplitude ratio change amount and phase difference change amount calculating means 1401 is configured to determine the sensing between the first receiving line ⁇ and the second receiving line ⁇ in the axial direction of the
  • the indication office The first and second measuring point selecting means 1400 reselect the measuring point.
  • the predetermined amplitude ratio change amount threshold value range may be 0-0.03 dB or other predetermined range, and the predetermined phase difference change amount threshold value range is 0°-0.1 ° or other predetermined range.
  • the second homogeneous formation selectable point determining device 1404 is coupled to the second amplitude ratio change amount and phase difference change amount calculating means 1402, and is configured to determine the axial direction of the logging device at the second measuring point Whether the amplitude ratio change amount and the phase difference change amount A PSD of the induced electromotive force between the first receiving line ⁇ and the second receiving coil are within their respective predetermined threshold ranges, and if so, the second measuring point is taken as the first
  • the optional points of the two homogeneous formations are stored in the storage device 1405. If not, the first and second measurement point selection means 1400 are instructed to reselect the measurement point.
  • the base value determining device 1406 is coupled to the storage device 1405 and configured to determine an amplitude ratio of the sensing signal of the logging device corresponding to the formation resistivity of the measured high resistance target layer to a base value of 0 and a phase difference base value 3 ⁇ 4£»o. According to a preferred embodiment, the base value determining means 1406 senses the induced electromotive force between the first receiving coil and the second receiving coil at the first and second homogeneous formation selectable points stored in the storage means 1405.
  • the average of the amplitude ratios (average of multiple amplitude ratios for each measurement made at the optional points of the two homogeneous formations) or the average of the root mean square and phase difference (in two homogeneous formations)
  • the average value of the plurality of phase differences obtained by each measurement at the optional point or the root mean square is respectively used as the amplitude ratio base value ⁇ "0 and the phase difference base value corresponding to the formation resistivity of the measured high resistance target layer.
  • the base value determining means 1406 is calculated by a magnetic dipole source dyadic Green's function The formation resistivity, the amplitude ratio and the phase difference of the selectable points of the first and second homogeneous formations are calculated. It is to be noted that the base value determining means 1406 may also use other existing functions or algorithms to calculate the formation resistivity, amplitude ratio and phase difference of the selectable points of the first and second homogeneous formations.
  • the standard value determining means 1407 is coupled to the base value determining means 1406 and the storage means 1405 and is used to determine and store a standard value of the formation resistivity of the measured high resistance target layer. According to a preferred embodiment, the standard value determining means 1407 is adapted to compare the amplitude ratio base value and phase difference base value corresponding to the formation resistivity of the measured high resistance target layer with corresponding predetermined eigenvalues of various formations. Selecting an eigenvalue of the type of the layer closest to the base value and the phase difference base value as the amplitude ratio standard value and phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer And storing the amplitude in the storage device 1405 in comparison with the standard value and the phase difference standard value.
  • the exit threshold setting means 1408 is coupled to the standard value determining means 1407 and the storage means 1405 and is used to set the exit threshold of the measured high resistance target layer. According to a preferred embodiment, the exit layer threshold setting means 1408 sets the output of the measured high resistance target layer according to an amplitude ratio standard value and a phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer. The layer threshold is then preferably stored in the storage device 1405.
  • the amplitude ratio and the phase difference of the induced electromotive force between the first receiving line ⁇ and the second receiving line ⁇ in the axial direction of the logging device are caused.
  • the predetermined value is the exit threshold as described herein.
  • the threshold of the egress layer can be set to different predetermined values according to the characteristics and measurement conditions of the actual measurement stratum for the different measurement strata by the person skilled in the art, generally through the two layers of the current measured stratum and the front stratum.
  • the resistivity contrast is determined.
  • the exit threshold can be set to an amplitude ratio of 1% of the standard value or the phase difference standard value regardless of the resistivity contrast of the two layers of the current measured formation and the front formation. 30%;
  • the layer threshold may preferably be set to 10% of the amplitude ratio standard value or phase difference standard value.
  • the third-nth measurement point selection and calculation device 1409 is configured to continue to select the next measurement point, perform at least two measurements at the next measurement point, and calculate the first direction along the axial direction of the logging device at the measurement point.
  • the low resistance formation determining means 1410 is coupled to the storage means 1405, the exit threshold setting means 1408 and the third - nth measuring point selecting and calculating means 1409, respectively.
  • the low-resistance formation determining device 1410 includes a layering threshold determining unit 14101 for determining a change in the amplitude ratio of the current measuring point calculated in the third-nth measuring point selection and computing device 1409. Whether the quantity ⁇ and the phase difference change amount A PSD is greater than the exit threshold; if it is greater, it is determined that the front of the logging device is a low-resistance formation; if not, the amplitude ratio of the current measurement point is preferably changed and phase The difference variation A PSD is stored in the storage device 1405.
  • the low-resistance formation determining means 1410 further includes a measuring point number determining unit 14102 and an amplitude ratio and phase difference changing tendency determining unit 14103.
  • the measurement point number determining unit 14102 is configured to determine whether the current measurement point has reached the predetermined time when the out-of-layer threshold value determining unit 14101 determines that the amplitude ratio change amount and the phase difference change amount A PSD of the current measurement point are not greater than the exit threshold value.
  • the nth measurement point if not, instructs the third-nth measurement point selection and calculation device 1409 to continue the selection of the next measurement point and the amplitude ratio change amount ⁇ " and the phase difference variation A PSD
  • the indication amplitude ratio and phase difference change trend determining unit 14103 is based on the previously stored measurement points (ie, 3, 4, 5... ⁇
  • the amplitude ratio change amount ⁇ " and the phase difference change amount A PSD at the measurement point) determine the amplitude ratio change tendency and the phase difference change tendency.
  • is selected by the technician according to the actual conditions of the formation according to the characteristics of the formation and the measured speed. For example, if for a softer formation (such as sandstone in the Bohai area), the value of ⁇ can be Relatively small, and for harder formations (such as shale), the value of ⁇ can be relatively large. Generally, for ordinary formations, ⁇ is preferably 20-30, but the present invention never Limits to this, it can be other suitable values.
  • the low-resistance formation determining device 1410 further includes a co-directional incremental change trend determining unit 14104, wherein the co-directional incremental change trend determining unit 14104 is configured to determine that the amplitude ratio and the phase difference change trend are determined.
  • the change determined by unit 14103 Whether the trend is from the third measurement point to the nth measurement point, the amplitude ratio change amount and the phase difference change amount keep increasing in the same direction (that is, the amplitude ratio change amount and phase difference change at the m+1 measurement point)
  • the low-resistance formation determining device 1410 further includes an overall in-situ incremental change trend determining unit 14105, configured to determine whether the change trend is the same when the determination result of the determining unit 14104 is negative. The direction is incremented, and if so, it is determined that the front of the logging device is a low resistance formation; if not, it is determined that no low resistance formation is present in front of the logging device.
  • the overall in-situ increment here means: although there is an ups and downs in the middle of the trend (that is, the amplitude ratio change and the phase difference change at a certain measurement point are relative to the previous measurement point).
  • the amplitude is smaller than the amount of change and the amount of phase difference change), but for example, at least 70% of the measurement points maintain a trend of increasing in the same direction, which is also preset by the technician based on the actual measurement.
  • the 70% is merely exemplary and does not constitute a limitation of the scope of the present invention.
  • the preferred embodiment can be implemented in hardware, software, firmware or a combination thereof.
  • the device components are implemented in software or firmware stored in a memory and executed by a suitable instruction execution system. If implemented in hardware, as in some embodiments, the device components can be implemented with any of the following techniques or combinations thereof well known in the art: having a logic gate for implementing logic functions on data signals (one or Multiple) discrete logic circuits, application specific integrated circuits (ASICs) with appropriate combinational logic gates, programmable gate array(s) (PGA), field programmable gate arrays (FPGAs), and more.
  • ASICs application specific integrated circuits
  • PGA programmable gate array
  • FPGAs field programmable gate arrays
  • a software component can include an ordered list of executable instructions for implementing logical functions, which can be embodied in any computer readable medium for use by or in connection with an instruction execution system, apparatus, or device, the instruction execution system A device or device, such as a computer-based system, a system containing a processor, or other system capable of acquiring instructions from an instruction execution system, apparatus, or device and executing the instructions. Further, the scope of the present disclosure includes the functionality of one or more embodiments embodied in logic embodied in a hardware or software constructed medium.

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Abstract

A well logging device, a well logging method and a data processing apparatus therefor are provided. The well logging device comprises a drill collar body and an antenna array. The antenna array comprises at least one pair of transmitting antenna and receiving antenna, and the transmitting antenna and the receiving antenna are used for generating a forward detection depth curve. By use of the well logging method, not only can the change of the forward stratum resistivity of the well drilling be measured in real time in a well drilling process, but also characteristics of different resistivity stratum interfaces in the forward direction can be distinguished in the drillingprocess.

Description

一种测井装置、 测井方法及数据处理设备 技术领域  Logging device, logging method and data processing device
本发明涉及测井技术领域, 更具体地, 本发明涉及钻井行业的随 钻测量技术领域, 特别是, 本发明涉及一种在钻井工程中用于地质导 向的测井装置、 测井方法以及相应的数据处理设备。 背景技术  The present invention relates to the field of logging technology, and more particularly, the present invention relates to the field of drilling while drilling technology, and in particular, the invention relates to a logging device, a logging method and a corresponding method for geosteering in a drilling engineering. Data processing equipment. Background technique
目前, 在诸如油气勘测、 煤层气、 在页岩地层中俘获的页岩气、 采煤等钻井行业的随钻测量领域中, 通常采用地层电阻率来形成地层 剖面图和确定储层的含油饱和度、 煤体结构的含气量及矿物断层, 因 此地层电阻率是测井解释评价油气、 煤、 矿产储藏的主要依据。 现在 已知的随钻电阻率测井技术包括随钻侧向电阻率测井、 随钻电磁波传 播电阻率测井和随钻感应电阻率测井。  At present, in the field of measurement while drilling in oil and gas exploration, coalbed methane, shale gas captured in shale formations, coal mining, etc., formation resistivity is often used to form stratigraphic profiles and determine reservoir oil saturation. Degree, gas content of coal structure and mineral faults, so formation resistivity is the main basis for logging interpretation and evaluation of oil and gas, coal and mineral storage. Known drilling-while-drilling resistivity logging techniques include LWD lateral resistivity logging, LWD electromagnetic transmission resistivity logging, and LWD induction resistivity logging.
随钻侧向电阻率测井装置的工作原理主要是由供电电极提供电 流, 在井眼周围地层中形成电场, 测量地层中电场的分布, 得出地层 电阻率。 随钻侧向电阻率测井装置将钻头本身作为电极, 也可以应用 环状电极和靠近钻头的 3 个纽扣电极进行电阻率测量。 在采用钻头作 为电极的情况下, 在泥浆侵入或井眼可能损坏之前, 随钻侧向电阻率 测井装置就可以测量 5 ~ 10厘米薄层的电阻率。 而如果采用 3 个钮扣 电极阵列, 则可进行高分辨率的侧向电阻率测量, 可减少围岩的影响, 甚至在盐水泥浆或高电阻率地层中也可以提供地层真电阻率响应。 此 外, 如果应用环状电极, 则可获得井眼周围 360° 范围的电阻率信息。  The working principle of the lateral resistivity logging device while drilling is mainly to provide current by the power supply electrode, form an electric field in the formation around the wellbore, measure the distribution of the electric field in the formation, and obtain the formation resistivity. The while-drilling lateral resistivity logging device uses the drill bit itself as an electrode. It is also possible to use a ring electrode and three button electrodes close to the drill bit for resistivity measurement. With the drill bit as the electrode, the LWD lateral resistivity logging device can measure the resistivity of a 5-10 cm thin layer before the mud intrusion or the wellbore may be damaged. With three button electrode arrays, high-resolution lateral resistivity measurements can be made to reduce the effects of surrounding rock and provide true resistivity response even in salt grout or high resistivity formations. In addition, if a ring electrode is applied, resistivity information in the 360° range around the wellbore can be obtained.
然而, 随钻侧向电阻率测井装置存在如下缺点: 因为侧向电阻率 测井属于直流电法测井, 首先要有一个供电电极将直流电流导入地层, 然后用一个测量电极测出井内某点的电位, 所以只有当井内有导电泥 浆提供电流通道时才能使用这种侧向电阻率测井方法。 然而在实际钻 井作业过程中, 例如在石油钻井过程中, 有时为了获取地层原始含油 饱和度信息, 需要采用油基泥浆钻井, 甚至采用空气钻井, 而在这种 条件下, 则不能使用直流电法测井, 即随钻侧向电阻率测井方法在这 些情况下变得不再适用。  However, the LWD lateral logging resisting device has the following disadvantages: Because the lateral resistivity logging is a DC logging, the first step is to have a supply electrode to direct the DC current into the formation, and then use a measuring electrode to measure a point in the well. The potential, so this lateral resistivity logging method can only be used when there is conductive mud in the well to provide a current path. However, during actual drilling operations, such as during oil drilling, sometimes oil-based mud drilling is required to obtain the original oil saturation information of the formation, even using air drilling. Under such conditions, direct current measurement cannot be used. Wells, ie, while drilling lateral resistivity logging methods, are no longer applicable in these situations.
随钻电磁波传播电阻率测井装置采用多线圏系设计, 传播频率为 1 ~ 8MHz, 线圈系基于钻铤本体结构, 将线圈系缠绕在钻铤上, 通过 测量不同源距接收线圏间幅度比或相位差, 然后再换算为地层视电阻 率, 测得相移浅电阻率和衰减深电阻率。 在理想情况下, 随钻电磁波 传播电阻率测井装置的纵向分辨率由两接收线圈的间距决定, 多探测 深度的测量数据可以用来解释侵入状况,通常认为相位电阻率的探测深 度较浅, 衰减电阻率具有较大的探测深度。 The electromagnetic wave propagation resistivity logging device while drilling uses a multi-wire tether design with a propagation frequency of 1 ~ 8MHz, the coil is based on the body structure of the drill collar, and the coil system is wound on the drill collar. By measuring the amplitude ratio or phase difference between the different source distances of the receiving line, and then converting to the apparent resistivity of the formation, the phase shift is measured shallow. Resistivity and attenuation of deep resistivity. Ideally, the longitudinal resolution of the electromagnetic wave propagation resistivity logging device is determined by the spacing of the two receiving coils. The measurement data of the multiple detection depths can be used to explain the intrusion condition. It is generally considered that the phase resistivity is shallow. The decay resistivity has a large depth of detection.
公开号为 CN101609169A、题为 "一种提高电磁波电阻率测量精度 和扩展其测量范围的方法" 的参考文献公开了通过对发射天线和接收 天线之间互感电动势进行计算, 消除了互感电动势的幅度衰减一电阻 率转换图和相位差-电阻率转换图中与地层电阻率无关的互感电动势、 电路零信号、 天线系统基值信号, 计算获得相位差及幅度衰减对地层 电阻率的转换。  The publication entitled CN101609169A, entitled "A Method for Improving the Measurement Accuracy of Electromagnetic Wave Resistivity and Extending the Measurement Range" discloses the calculation of the mutual inductance electromotive force between the transmitting antenna and the receiving antenna, eliminating the amplitude attenuation of the mutual inductance electromotive force. A resistivity conversion diagram and a phase difference-resistivity conversion diagram are the mutual inductance electromotive force, the circuit zero signal, and the antenna system base value signal independent of the formation resistivity, and the phase difference and the amplitude attenuation are converted to the formation resistivity.
此外, 发表于中国石油大学学报的文献 "倾斜线圈随钻电磁波电 阻率测量仪器基本原理及其在地质导向中的应用" 采用各向异性水平 层状介质的磁偶极源并矢 green 函数计算倾斜线圈随钻电磁波电阻率 测量仪器的响应, 分析井眼相对倾角和接收线圏倾斜角对接收信号幅 度比和相位差的影响, 以及传统仪器和新型仪器在垂直于仪器轴方向 的响应曲线角峰的性质, 从而更早地预测到地层边界的存在。  In addition, the paper published in the Journal of China University of Petroleum, "The basic principle of the electromagnetic coil resistivity measuring instrument for tilting coils while drilling and its application in geosteering" uses the magnetic dipole source of the anisotropic horizontal layered medium to calculate the tilt The response of the coil electromagnetic wave resistivity measuring instrument while drilling, analyzing the influence of the relative inclination angle of the wellbore and the inclination angle of the receiving line on the amplitude ratio and phase difference of the received signal, and the peak of the response curve of the conventional instrument and the new instrument in the direction perpendicular to the instrument axis The nature of the formation, thus predicting the existence of stratigraphic boundaries earlier.
然而, 尽管现有的各种随钻电磁波传播电阻率测井装置能够测得 不同探测深度的电阻率, 但现有的各种随钻电磁波传播电阻率测井装 置存在如下缺点: 首先, 随钻电磁波传播电阻率测井装置采用的信号 频率太高, 由于电磁波的传播效应, 所以其探测深度有限。 其次, 随 钻电磁波传播电阻率测井装置的测量结果会受到地质因素的影响, 尤 其是围岩的影响, 因为装置的测量结果并不仅限于接收线圈之间的地 层区域, 而且与发射线圈到接收线圏之间的整个地层参数有关, 甚至 于发射线圏周围一个较小区域内的地层也会对测量结果产生影响, 所 以该测井装置的纵向分辨率在很大程度上依赖于整个装置所处地层的 电阻率。 第三, 由于随钻电磁波传播电阻率测井装置的线圏系是缠绕 在钻铤表面的, 所以其制作工艺非常复杂, 而且在使用过程中线圈系 极容易受到磨损而损坏, 并且当井眼尺寸变化时, 需要重新绕制线圈, 维修检测较为复杂, 维护成本高。 此外, 与随钻侧向电阻率测井装置 类似, 随钻电磁波传播电阻率测井装置也不能工作在油基泥浆中。 随钻感应电阻率测井装置利用电磁感应原理, 当在发射线圏中施 加幅度和频率恒定的交流电时, 在该线圈的周围地层中感应出涡流, 涡流本身又会形成二次交变电磁场, 在二次交变电磁场作用下, 接收 线圈中产生感应电动势, 该电动势大小与地层电导率有关, 通过测量 感应电动势即可得到地层电阻率。 However, although various existing electromagnetic wave propagation resistivity logging devices capable of measuring electromagnetic wave resistance resistivity can measure resistivity of different detection depths, the existing various electromagnetic wave propagation resistivity logging devices while drilling have the following disadvantages: First, while drilling The electromagnetic wave propagation resistivity logging device uses a signal frequency that is too high, and its detection depth is limited due to the electromagnetic wave propagation effect. Secondly, the measurement results of the electromagnetic wave propagation resistivity logging device while drilling will be affected by geological factors, especially the surrounding rock, because the measurement results of the device are not limited to the formation area between the receiving coils, and the transmitting coil to the receiving The entire formation parameter between the turns is related, even the formation in a smaller area around the launch line will have an impact on the measurement results, so the vertical resolution of the logging device depends to a large extent on the entire device. The resistivity of the formation. Third, since the wire-wound system of the electromagnetic wave-transmitting resistivity logging device is wound around the surface of the drill collar, the manufacturing process is very complicated, and the coil system is extremely susceptible to wear and damage during use, and when the well is drilled When the size changes, the coil needs to be re-rolled, and the maintenance inspection is complicated and the maintenance cost is high. In addition, similar to the lateral resistivity logging device while drilling, the electromagnetic wave propagation resistivity logging device cannot be operated in oil-based mud. The on-board induction resistivity logging device utilizes the principle of electromagnetic induction. When an alternating current of constant amplitude and frequency is applied to the emission line, an eddy current is induced in the surrounding formation of the coil, and the eddy current itself forms a secondary alternating electromagnetic field. Under the action of the secondary alternating electromagnetic field, an induced electromotive force is generated in the receiving coil. The magnitude of the electromotive force is related to the conductivity of the formation. The formation resistivity can be obtained by measuring the induced electromotive force.
目前的随钻感应电阻率测井装置的线圈系采用一个发射线圈和两 个接收线圈, 所述两个接收线圈中的一个为主接收线圈, 另一个为补 偿线圏, 线圏系置于钻铤侧面带有反射层的 V形槽内, 测井响应对 V 形槽正面区域地层的电阻率变化敏感, 因此具有定向测量的特点。 随 钻感应电阻率测井装置由电池供电, 在电池顶部装有一个公扣连接头, 该公扣连接头可与随钻感应电阻率测井装置底部的母扣连接头相接, 用于向随钻感应电阻率测井装置传送实时数据, 同一个传感器短节可 适用于不同尺寸井眼的要求。  At present, the coil of the induction-resistance resistivity logging device adopts one transmitting coil and two receiving coils, one of the two receiving coils is a main receiving coil, and the other is a compensating coil, and the coil is placed on the drill. In the V-shaped groove with the reflective layer on the side, the logging response is sensitive to the resistivity change of the formation in the front area of the V-shaped groove, and therefore has the characteristics of directional measurement. The while-drilling resistivity logging device is powered by a battery, and a male snap connector is attached to the top of the battery. The male snap connector can be connected to the female snap connector at the bottom of the LWD logging device for The LWD inductive resistivity logging device delivers real-time data, and the same sensor sub-section can be used for different sizes of wellbore requirements.
这种随钻感应电阻率测井装置的优点是: 其信号频率为 20kHz, 大 大低于高频装置的频率, 因此不易被地层吸收, 探测深度深, 测量范 围较大, 可达到 0.1-1000 欧姆米, 而且其结构设计简单, 一个传感器 短节可适用于不同尺寸井眼的需要, 维修检测简单, 且适用不同类型 的钻井液。  The advantages of this MWD logging device are: The signal frequency is 20 kHz, which is much lower than the frequency of the high frequency device, so it is not easily absorbed by the formation. The depth of detection is deep and the measurement range is large, which can reach 0.1-1000 ohms. M, and its structural design is simple, a sensor sub-section can be applied to the needs of different sizes of wells, maintenance inspection is simple, and different types of drilling fluids are applicable.
然而, 这种随钻感应电阻率测井装置还存在如下缺点: 由于该装 置采用由一个发射线圈和两个接收线圏组成的、 具有单一固定探测深 度的线圈系, 所以该测井装置只能提供一个径向探测深度的地层电阻 率, 不能用于解释复杂侵入剖面和划分渗透层。 此外, 对于渗透层而 言, 泥浆侵入使其电阻率在径向上发生变化, 由于在同一深度点只能 得到一个径向探测深度的电阻率值, 因此随钻感应电阻率测井装置不 能用来解释地层侵入状况, 无法确定地层受泥浆侵入的情况和储层渗 透性, 不利于油气层解释, 从而无法用来准确测量地层真电阻率。 另 外, 对于不同类型的泥浆侵入以及不同径向探测深度的电阻率而言, 其油气水层特征是不同的, 根据多条不同探测深度电阻率曲线受泥浆 侵入影响程度的不同、 以及在油气水层中所表现出来的差异特征可以 识别油气, 所以多深度电阻率测量对于随钻测井装置来说是非常重要 的, 然而目前的这种随钻感应电阻率测井装置却无法达到这个要求, 因为它的线圈系设计结构固定, 每一种线圏系只能提供一种深度的电 阻率, 要得到不同探测深度的电阻率, 就得用不同的线圈系进行多次 是很难实现的。 ^ : ' ^ ^ However, such a Drilling Induction Resistivity Logging Device has the following disadvantages: Since the device employs a coil system consisting of one transmitting coil and two receiving turns with a single fixed depth of detection, the logging device can only Providing a formation resistivity with a radial depth of investigation cannot be used to explain complex intrusion profiles and to divide the permeable layer. In addition, for the permeable layer, the mud intrusion causes the resistivity to change radially. Since only one radial detection depth resistivity value can be obtained at the same depth point, the LWD induction logging device cannot be used. Explain the situation of stratum intrusion, it is impossible to determine the situation of reservoir intrusion by mud and reservoir permeability, which is not conducive to the interpretation of oil and gas layers, and thus cannot be used to accurately measure the true resistivity of the formation. In addition, for different types of mud intrusion and resistivity of different radial depths, the characteristics of the oil and gas layers are different. According to the different degrees of different depths, the resistivity curve is affected by the mud intrusion, and the oil and gas The difference characteristics exhibited in the layer can identify oil and gas, so multi-depth resistivity measurement is very important for the logging while drilling device. However, the current Drilling Induction Resistivity Logging Device cannot meet this requirement. Because its coil system design structure is fixed, each type of wire can only provide one depth of electricity. Resistivity, to obtain resistivity at different depths of detection, it is difficult to achieve multiple times with different coil systems. ^ : ' ^ ^
综上所述, 无论是上述哪种随钻电阻率测井装置, 其都存在诸多 缺陷, 并且, 上述各种随钻电阻率测井装置都只致力于径向探测深度 的方法研究和计算, 而并未提及或涉及到前向探测深度。 然而, 随着 各类随钻电阻率测井装置的发射天线和接收天线的数量的不断增多,发 射频率降低,前向深度探测对于钻井工程而言变得越来越重要,因此, 目 前在钻井测井领域中对于随钻前向探测方法的需求变得愈来愈迫切。 发明内容: 陷, 本发明提供了一种新的随钻测井方法, 该方法在钻井过程中不但 能够实时测量钻井前向地层电阻率变化, 还能够分辨钻进过程中前方 不同的电阻率层界面特征。  In summary, no matter which of the above-mentioned while-resistance resistivity logging devices, there are many defects, and the above-mentioned various LWD resistivity logging devices are only devoted to the method research and calculation of the radial depth of detection. There is no mention or involvement in forward detection depth. However, as the number of transmitting and receiving antennas of various types of LWD logging devices continues to increase, the transmission frequency decreases, and forward depth detection becomes more and more important for drilling engineering. Therefore, drilling is currently underway. The need for a forward-while-drilling method in the logging field is becoming more and more urgent. SUMMARY OF THE INVENTION: The present invention provides a new logging while drilling method, which can not only measure the forward resistivity change of the well in real time during the drilling process, but also distinguish different resistivity layers in front of the drilling process. Interface features.
根据本发明的一个方面, 提供了一种测井方法, 其包括:  According to an aspect of the invention, a logging method is provided, comprising:
( a ) 均质测量点选取步骤, 在该步骤中, 使测井装置选取两个 连续测量点来进行至少两次连续测量;  (a) a homogeneous measurement point selection step in which the logging device selects two consecutive measurement points for at least two consecutive measurements;
( b ) 根据所述两个连续测量点处的测量结果来确定所选取的所 I 述两个连续测量点是否均能作为均质地层可选点; 如果是, 则  (b) determining, based on the measurements at the two consecutive measurement points, whether the selected two consecutive measurement points are capable of being a homogeneous formation selectable point; if so,
( c ) 根据两个所述均质地层可选点来确定与所测高阻目的层的 地层电阻率相对应的所述测井装置的感应信号的幅度比基值和相位差 基值;  (c) determining, according to the two selected points of the homogeneous formation, an amplitude ratio base value and a phase difference base value of the sensing signal of the logging device corresponding to the formation resistivity of the measured high resistance target layer;
( d ) 根据所述幅度比基值和相位差基值来确定与所测高阻目的 , 层的地层电阻率相对应的幅度比标准值和相位差标准值;  (d) determining, according to the amplitude ratio base value and the phase difference base value, a magnitude ratio standard value and a phase difference standard value corresponding to the measured resistivity of the layer;
( e ) 根据所述幅度比标准值和相位差标准值来设定所述所测高 阻目的层的出层阔值;  (e) setting an exit threshold of the measured high resistance target layer according to the amplitude ratio standard value and the phase difference standard value;
( f ) 继续选取下一个测量点进行至少两次测量;  (f) continue to select the next measurement point for at least two measurements;
( g ) 判断在当前测量点处、 测井装置的一对接收线圈之间的感 • 应电动势的幅度比变化量和 /或相位差变化量是否大于所述出层阈值;  (g) determining whether the sense of the amplitude of the electromotive force and/or the amount of change in the phase difference between the pair of receiving coils of the logging device at the current measuring point is greater than the threshold of the exiting layer;
( h ) 如果步骤 (g ) 的判断结果为是, 则判定测井装置前方出现 低阻地层。 根据本发明的另一个方面, 提供了一种数据处理设备, 其特征在 于, 该数据处理设备包括: (h) If the result of the determination in step (g) is YES, it is determined that a low-resistance formation appears in front of the logging device. According to another aspect of the present invention, a data processing device is provided, characterized in that the data processing device comprises:
均质地层可选点判定装置 ( 1403、 1404 ) , 其用于判定测井装置 当前所选取的两个连续测量点是否均能作为均质地层可选点;  The homogeneous formation optional point determining device (1403, 1404) is used for determining whether two consecutive measuring points currently selected by the logging device can be used as the selective points of the homogeneous formation;
基值确定装置 ( 1406 ) , 其用于在所述均质地层可选点判定装置 ( 1403、 1404 ) 的判断结果为是的情况下, 根据两个所述均质地层可 选点来确定与所测高阻目的层的地层电阻率相对应的所述测井装置的 感应信号的幅度比基值和相位差基值;  a base value determining device (1406) for determining, based on the two selectable points of the homogeneous formation layer, if the determination result of the homogeneous formation point selectable device (1403, 1404) is YES The amplitude of the induced signal of the logging device corresponding to the formation resistivity of the measured high resistance target layer is greater than the base value and the phase difference base value;
标准值确定装置 ( 1407 ) , 其用于根据所述幅度比基值和相位差 基值来确定与所测高阻目的层的地层电阻率相对应的幅度比标准值和 相位差标准值;  a standard value determining device (1407) for determining an amplitude ratio standard value and a phase difference standard value corresponding to a formation resistivity of the measured high resistance target layer according to the amplitude ratio base value and the phase difference base value;
出层阈值设定装置 ( 1408 ) , 其用于根据所述幅度比标准值和相 位差标准值来设定所述所测高阻目的层的出层阔值;  a layer threshold setting device (1408) configured to set an exit threshold of the measured high resistance target layer according to the amplitude ratio standard value and a phase difference standard value;
第三一第 n 测量点选取及计算装置 ( 1409 ) , 其用于继续选取下 一个测量点进行至少两次测量, 并计算在当前所选取的测量点处、 测 井装置的一对接收线圈之间的感应电动势的幅度比变化量和相位差变 化量; 以及  a third-th nth measuring point selection and calculating device (1409) for continuously selecting the next measuring point for at least two measurements, and calculating a pair of receiving coils of the logging device at the currently selected measuring point The magnitude of the induced electromotive force between the amount of change and the amount of change in phase difference;
低阻地层判定装置( 1410 ) , 其包括出层阈值判定单元( 14101 ) , 该单元用于判断所述当前所选取的测量点处的幅度比变化量和 /或相位 差变化量是否大于所述出层阈值; 如果是, 则判定测井装置前方出现 低阻地层。  a low-resistance formation determining device (1410), comprising an out-of-layer threshold determining unit (14101), configured to determine whether an amplitude ratio change amount and/or a phase difference change amount at the currently selected measurement point is greater than The exit threshold; if so, it is determined that a low-resistance formation is present in front of the logging device.
根据本发明的再一个方面, 提供了测井装置, 其特征在于, 所迷 测井装置包括钻铤本体 ( 12 ) 和天线阵列, 其中所述天线阵列包括至 少一对发射天线和接收天线, 所述发射天线和接收天线用于生成前向 探测深度曲线。  According to still another aspect of the present invention, there is provided a logging apparatus, characterized in that the logging apparatus comprises a drill collar body (12) and an antenna array, wherein the antenna array comprises at least one pair of transmitting antennas and receiving antennas, The transmit and receive antennas are used to generate a forward detected depth profile.
相比较径向深度探测而言, 根据本发明的前向深度探测具有下列 重要意义:首先, 根据本发明的前向深度探测可有效地控制钻井工程造 斜段轨迹; 公知的水平段测量地层通常是先假定水平层状分布, 当开 始造斜时, 电阻率测井装置与这些水平层状地层近乎垂直, 因而径向 探测响应只能反映某个层面的测量地层的电阻率变化情况, 而前向探 测响应却具有多个前向探测深度, 其可反映不同的钻井深度上的测量 地层的电阻率变化, 可以有效识别层边界和油水触面, 调整造斜弧度 使之准确平滑, 进而保证造斜段钻井质量。 其次, 当钻井进入复杂的 大斜度井或水平井段时, 根据本发明的前向深度探测可对钻井前端地 层进行不同深度的前向探测, 其比径向探测方法更直接和准确, 可预 先判断薄油层、 复杂褶皱及互夹层, 从而有效绕开断层以及沿高 dip储 层长距离钻进, 获得最高油气有效钻遇率。 Compared to radial depth detection, the forward depth detection according to the present invention has the following important significance: First, the forward depth detection according to the present invention can effectively control the trajectory of the drilling engineering slant section; the well-known horizontal section measurement formation usually The horizontal layered distribution is assumed first. When the slanting is started, the resistivity logging device is nearly perpendicular to the horizontal layered strata, so the radial detection response can only reflect the change of the resistivity of the measured formation at a certain level. The response to the probe has multiple forward detection depths, which reflect the change in resistivity of the measured formation at different depths of the well, which can effectively identify the layer boundary and the oil-water contact, and adjust the oblique curvature. Make it accurate and smooth, and thus ensure the quality of drilling in the inclined section. Secondly, when the drilling enters a complex high-angle well or horizontal well section, the forward depth detection according to the present invention can perform forward detection of different depths on the front end of the drilling well, which is more direct and accurate than the radial detection method. Pre-determine thin oil layers, complex folds and mutual interlayers, so as to effectively bypass the faults and drill long distances along the high dip reservoir to obtain the highest oil and gas effective drilling rate.
根据本发明的测井方法及相应的数据处理装置可以在钻井过程中 实时地测量地层的电阻率变化率的变化特征, 实时分辨地层界面及油 水界面, 捕捉进入油气储集层的最佳时机, 并且在高地层倾角及各向 异性地层水平井中, 能够长距离预测钻头前方地质信息并及时调整井 眼轨迹, 控制钻具穿行在油藏最佳位置, 从而获得最大触油面, 非常 适合于在石油工程中进行地质导向。 附图说明:  The logging method and the corresponding data processing device according to the present invention can measure the change characteristics of the resistivity change rate of the formation in real time during the drilling process, and accurately resolve the formation interface and the oil-water interface in real time, and capture the optimal timing of entering the oil and gas reservoir. In the high-level dip angle and the anisotropic formation horizontal well, the geological information in front of the drill bit can be predicted for a long distance and the well trajectory can be adjusted in time to control the drilling tool to travel through the optimal position of the reservoir, so as to obtain the maximum oil-touch surface, which is very suitable for Geosteering in petroleum engineering. BRIEF DESCRIPTION OF THE DRAWINGS:
图 1示出了根据本发明优选实施例的测井装置;  Figure 1 shows a logging device in accordance with a preferred embodiment of the present invention;
图 2示出了根据本发明的测井方法所采用的二层地层模型图; 图 3示出了电阻率对比度为 10/1地层幅度衰减响应随地层界面位 置的变化关系图;  Figure 2 is a diagram showing a two-layer formation model used in the logging method according to the present invention; Figure 3 is a graph showing the relationship between the amplitude attenuation response of the formation and the position of the formation interface with a resistivity contrast of 10/1;
图 4示出了电阻率对比度为 10/1地层相位移响应随地层界面位置 的变化关系图;  Figure 4 shows the relationship between the displacement response of the formation with the resistivity contrast of 10/1 and the position of the formation interface;
图 5示出了电阻率对比度为 50/1地层幅度衰减响应随地层界面位 置的变化关系图;  Figure 5 shows the relationship between the amplitude attenuation response of the formation with a resistivity contrast of 50/1 and the position of the formation interface;
图 6示出了电阻率对比度为 50/1地层相位移响应随地层界面位置 的变化关系图;  Figure 6 shows the relationship between the displacement response of the formation with the resistivity contrast of 50/1 and the position of the formation interface;
图 7示出了电阻率对比度为 200/1地层幅度衰减响应随地层界面位 置的变化关系图;  Figure 7 is a graph showing the relationship between the amplitude attenuation response of the formation and the position of the formation interface with a resistivity contrast of 200/1;
图 8示出了电阻率对比度为 200/1地层相位移响应随地层界面位置 的变化关系图;  Figure 8 is a graph showing the relationship between the displacement response of the formation and the position of the formation interface with the resistivity contrast of 200/1;
图 9 示出了根据本发明优选实施例的测井装置中的天线系 T2-R1 -R2在 2MHz的发射频率下的各种测量地层电阻率与幅度比和相 位差的本征值的对照表;  9 is a comparison table of various measured formation resistivity and amplitude ratios and phase difference eigenvalues of the antenna system T2-R1 - R2 in the logging device according to a preferred embodiment of the present invention at a transmission frequency of 2 MHz. ;
图 10 示出了根据本发明优选实施例的测井装置中的天线系 T2-R1 -R2在 400kHz的发射频率下的各种测量地层电阻率与幅度比和 相位差的本征值的对照表; Figure 10 illustrates various measured formation resistivity and amplitude ratios of antenna systems T2-R1 - R2 in a logging device in accordance with a preferred embodiment of the present invention at an emission frequency of 400 kHz. a comparison table of eigenvalues of phase differences;
图 1 1 示出了根据本发明优选实施例的测井装置中的天线系 T1 -R1 -R2在 2MHz的发射频率下的各种测量地层电阻率与幅度比和相 位差的本征值的对照表;  Figure 1 1 shows a comparison of various measured formation resistivity versus amplitude ratios and eigenvalues of phase differences for antenna systems T1 - R1 - R2 in a logging device in accordance with a preferred embodiment of the present invention at a transmission frequency of 2 MHz. Table
图 12 示出了根据本发明优选实施例的测井装置中的天线系 T1 -R1-R2在 400kHz的发射频率下的各种测量地层电阻率与幅度比和 相位差的本征值的对照表;
Figure imgf000009_0001
具体实施方式:
Figure 12 is a table showing the measured values of formation resistivity versus amplitude ratio and phase difference of the antenna system T1 - R1 - R2 in the logging device in accordance with a preferred embodiment of the present invention at an emission frequency of 400 kHz. ;
Figure imgf000009_0001
detailed description:
某些术语在本申请文件中自始至终用来指示特定系统部件。 如本 领域的技术人员将认识到的那样, 通常可以用不同的名称来指示相同 的部件, 因而本申请文件不意图区别那些只是在名称上不同而不是在 功能方面不同的部件。 在本申请文件中, 以开放的形式使用术语 "包 括 (comprise ) ,, 、 "包含 (include ) " 和 "具有 (have ) " , 并且因 此应将其解释为意指 "包括但不限于... " 。 此外, 在本文中可能使用 的术语 "基本上" 、 "实质上" 或者 "近似地" 涉及行业所接受的对 相应术语的容差。 如在本文中可能采用的术语 "耦合" 包括直接耦合 和经由另外的组件、 元件、 电路、 或者模块的间接耦合, 其中对于间 接耦合来说, 介于其间的组件、 元件、 电路、 或模块不更改信号的信 息但是可调整其电流水平、 电压水平、和 /或功率水平。推断的耦合(例 如其中一个元件通过推断耦合至另一个元件) 包括以与 "耦合" 同样 的方式在两个元件之间的直接和间接的耦合。  Certain terms are used throughout this document to indicate specific system components. As will be recognized by those skilled in the art, the same components may be denoted by different names, and thus the present application is not intended to distinguish between components that differ only in name but not in function. In this application, the terms "comprise", ", "include" and "have" are used in an open form, and therefore should be interpreted to mean "including but not limited to: In addition, the terms "substantially", "substantially" or "approximately" as used herein may relate to tolerances accepted by the industry for the corresponding term. The term "coupling" as may be used herein includes Direct coupling and indirect coupling via additional components, components, circuits, or modules, where indirect coupling, components, components, circuits, or modules do not alter signal information but can adjust their current levels, voltages Horizontal, and/or power levels. Inferred coupling (eg, one element is inferred to another element by inference) includes direct and indirect coupling between two elements in the same manner as "coupling."
在以下说明中, 出于解释的目的, 阐述许多特定细节以便提供对 本发明的透彻理解。 然而, 对于本领域的技术人员来说将显而易见的 是, 可以在没有这些特定细节的情况下实施本发明的装置、 方法和设 备。 在本说明书中对 "实施例" 、 "示例" 或类似语言的提及意指结 合该实施例或示例所描述的特定特征、 结构或特性被包括在至少那一 个实施例或示例中, 但不一定会被包括在其它的实施例或示例中。 在 本说明书中的不同位置中的措辞 "在一个实施例中" 、 "在优选实施 例中,, 或类似措辞的各种实例并不必定全部涉及同一实施例。 In the following description, numerous specific details are set forth However, it will be apparent to those skilled in the art that the device, method and apparatus of the present invention may be practiced without these specific details. References to "invention", "example" or similar language in this specification means that a particular feature, structure, or characteristic described in connection with the embodiment or example is included in at least one embodiment or example, but not It must be included in other embodiments or examples. The wording in different positions in this specification is "in one embodiment", "in a preferred implementation The examples, or the like, are not necessarily all referring to the same embodiment.
下面结合优选实施例和说明书附图对本发明作进一步描述。  The invention is further described below in conjunction with the preferred embodiments and the drawings.
图 1 示出了根据本发明优选实施例的一种测井装置——电磁波传 播电阻率探测装置, 其包括钻铤本体 12、 天线阵列 7-1 1、 13-15、 内部 电子线路 (图中未示出) 以及用于耦合各部件的固化密封件。  1 shows a logging device, an electromagnetic wave propagation resistivity detecting device, comprising a drill collar body 12, an antenna array 7-1 1 , 13-15, an internal electronic circuit (in the figure) according to a preferred embodiment of the present invention. Not shown) and a cured seal for coupling the components.
如图 1 中所示, 钻铤本体 12在本实施例中优选地由一根圆柱形且 内有轴向贯通孔的不锈钢材料制成, 该钻铤本体 12的外表面上优选地 刻有多个优选为环形或椭环形的凹槽, 该凹槽用于安装发射天线或接 收天线。  As shown in Fig. 1, the drill collar body 12 is preferably made of a stainless steel material having a cylindrical shape and an axial through hole in the present embodiment, and the outer surface of the drill collar body 12 is preferably engraved with a large amount. Preferably, a ring or an elliptical groove is used to mount the transmitting or receiving antenna.
在图 1所示出的优选实施例中,天线阵列包括 4个发射天线 T1 (如 附图标记 1 1所示) 、 T2 (如附图标记 14所示) 、 T3 (如附图标记 13 所示) 和 T4 (如附图标记 15所示) , 以及 4个接收天线 R1 (如附图 标记 7所示) 、 R2 (如附图标记 8所示) 、 R3 (如附图标记 9所示) 和 R4 (如附图标记 10所示) 。  In the preferred embodiment illustrated in Figure 1, the antenna array comprises four transmit antennas T1 (as indicated by reference numeral 1), T2 (as indicated by reference numeral 14), and T3 (as indicated by reference numeral 13). Show) and T4 (as indicated by reference numeral 15), and 4 receiving antennas R1 (as indicated by reference numeral 7), R2 (as indicated by reference numeral 8), R3 (as indicated by reference numeral 9) ) and R4 (as indicated by reference numeral 10).
如图 1 所示,发射天线和接收天线从图 1的左侧至图 1 的右侧(即 为从钻挺本体 12的钻挺尾端到钻头端) 的排列顺序优选为: 接收天线 R3、 发射天线 T3、 发射天线 Tl、 接收天线 Rl、 接收天线 R2、 发射天 线 T2、 发射天线 Τ4、 和接收天线 R4。 其中, 在本优选实施例中, 接 收天线 R1和 R2之间的中点为测量点, 发射天线 Tl、 Τ2、 Τ3和 Τ4优 选地分别以该测量点为中心对称地安装。 接收天线 R1和 R2优选地是 安装角均为零的接收天线对, 而接收天线 R3和 R4为另一对以所述测 量点为对称中心的接收天线对, 如图 1所示, 该接收天线 R3和 R4优 选地位于钻铤的两端。 该接收天线 R3和 R4的安装角可以任意设置, 在本实施例中其被优选地 (但不仅限于)设置为 45° 和 -45° 。  As shown in FIG. 1, the order of arrangement of the transmitting antenna and the receiving antenna from the left side of FIG. 1 to the right side of FIG. 1 (ie, from the tail end of the drill collar body 12 to the drill bit end) is preferably: receiving antenna R3, A transmitting antenna T3, a transmitting antenna T1, a receiving antenna R1, a receiving antenna R2, a transmitting antenna T2, a transmitting antenna Τ4, and a receiving antenna R4. In the preferred embodiment, the midpoint between the receiving antennas R1 and R2 is a measuring point, and the transmitting antennas T1, Τ2, Τ3 and Τ4 are preferably symmetrically mounted around the measuring point, respectively. The receiving antennas R1 and R2 are preferably receiving antenna pairs with a mounting angle of zero, and the receiving antennas R3 and R4 are another pair of receiving antennas with the measuring point as a center of symmetry, as shown in FIG. R3 and R4 are preferably located at both ends of the drill collar. The mounting angles of the receiving antennas R3 and R4 can be arbitrarily set, and in the present embodiment, they are preferably, but not limited to, set to 45° and -45°.
对于任何一个发射天线与一对接收天线对(例如发射天线 T1与接 收天线 R1 和 R2 ) 而言, 当发射天线被激发时, 电磁信号通过周围地 层及钻铤本体传播, 经过地层反射及透射而在接收天线上产生电磁感 应信号, 该电磁感应信号经由接收天线进行信号采集, 然后经由内部 电子线路进行放大、 滤波等信号处理, 最后转化为传播地层的电阻率 的函数。 当该测井装置 (在本实施例中为电磁波传播电阻率探测装置) 在井下运行时, 如果该装置前方的地层电参数 (例如地层电阻率对比 度) 不变, 则就意味着没有层边界出现, 此时反射到接收天线上的电 磁信号就会不变, 而如果该装置前方的地层电参数改变, 则就意味着 有层边界出现, 此时反射到接收天线上的电磁信号将产生改变, 从而 产生一个信号差, 不断地对这个信号差进行采集计算, 则可获得前向 探测的距离。 For any one of the transmitting antennas and a pair of receiving antennas (for example, the transmitting antenna T1 and the receiving antennas R1 and R2), when the transmitting antenna is excited, the electromagnetic signal propagates through the surrounding ground and the drill collar body, and is reflected and transmitted through the ground layer. An electromagnetic induction signal is generated on the receiving antenna, and the electromagnetic induction signal is collected by the receiving antenna, then subjected to signal processing such as amplification and filtering via the internal electronic circuit, and finally converted into a function of the resistivity of the propagating formation. When the logging device (in this embodiment, the electromagnetic wave propagation resistivity detecting device) is operated downhole, if the formation electrical parameters (such as formation resistivity contrast) in front of the device are unchanged, it means that no layer boundary appears. , the electricity reflected to the receiving antenna at this time The magnetic signal will not change, and if the electrical parameters of the formation in front of the device change, it means that a layer boundary appears, and the electromagnetic signal reflected to the receiving antenna will change, resulting in a signal difference, constantly This signal difference is calculated and calculated, and the distance of forward detection can be obtained.
根据本发明的测井装置 (在本实施例中为电磁波传播电阻率探测 装置) 中的任意一个发射天线和任一组接收天线对的组合都可以产生 一条前向探测曲线, 通过对所有的前向探测曲线进行比较及处理, 可 以消除环境影响 (例如井眼影响) 和测量误差, 从而可以提高测井装 置的前向探测精度。  A combination of any of the transmitting antennas and any of the sets of receiving antennas in the logging device (in this embodiment, the electromagnetic wave propagation resistivity detecting device) can generate a forward detecting curve through all of the front Comparing and processing the detection curve can eliminate environmental influences (such as wellbore effects) and measurement errors, thereby improving the forward detection accuracy of the logging device.
下面, 将结合附图来详细描述根据本发明另一优选实施例的一种 特定的随钻测井方法。  Hereinafter, a specific logging while drilling method according to another preferred embodiment of the present invention will be described in detail with reference to the accompanying drawings.
如图 13所示, 根据本发明优选实施例的测井方法——电磁波传播 电阻率前向探测方法, 包括如下步骤:  As shown in FIG. 13, a logging method according to a preferred embodiment of the present invention - a method for forward detection of electromagnetic wave resistivity, includes the following steps:
在步骤 1301 中, 将随钻测井装置 (优选地例如图 1所示的电磁波 传播电阻率前向探测装置) 放置到某深度位置处的高阻目的层中, 在 测井装置持续钻进时该测井装置进行连续探测, 其探测方向与该测井 装置 (优选地为图 〗 所示的电磁波传播电阻率前向探测装置) 的轴向 移动方向一致。  In step 1301, a logging while drilling device (preferably, for example, an electromagnetic wave propagation resistivity forward detecting device shown in FIG. 1) is placed in a high resistance target layer at a certain depth position, while the logging device continues to drill. The logging device performs continuous detection with a direction of detection that coincides with the direction of axial movement of the logging device (preferably the electromagnetic wave propagation resistivity forward detecting device shown in the figure).
在步骤 1302中, 选取两个连续测量点 (例如第一测量点和第二测 量点) , 在每个测量点处进行至少两次连续测量。  In step 1302, two consecutive measurement points (e.g., a first measurement point and a second measurement point) are selected, and at least two consecutive measurements are taken at each measurement point.
在步骤 1303中, 如果在第一测量点处、 在所述至少两次连续测量 中沿测井装置轴向方向的第一接收线圏与第二接收线圏之间的感应电 动势的幅度比变化量 Δ^"和相位差变化量 A PSD 在其各自的预定阈值 范围 (例如: 预定幅度比变化量阔值范围可以为 0-0.03dB或其他预定 范围,预定相位差变化量阈值范围为 0°-0. 1°或其他预定范围) 内, 则将 该第一测量点作为第一均质地层可选点保存。  In step 1303, if the amplitude ratio of the induced electromotive force between the first receiving line and the second receiving line in the axial direction of the logging device in the at least two consecutive measurements at the first measuring point is changed The quantity Δ^" and the phase difference change amount A PSD are in their respective predetermined threshold ranges (for example, the predetermined amplitude ratio variation amount threshold value may be 0-0.03 dB or other predetermined range, and the predetermined phase difference variation amount threshold value range is 0° Within -0. 1° or other predetermined range), the first measurement point is saved as a select point of the first homogeneous formation.
在步骤 1304中, 如果在第二测量点处、 在所述至少两次连续测量 中沿测井装置轴向方向的第一接收线圏与第二接收线圏之间的感应电 动势的幅度比变化量 ^1"和相位差变化量 A PSD 都在所述各自的预定 阈值范围内, 则将该第二测量点作为第二均质地层可选点保存。 In step 1304, if the amplitude ratio of the induced electromotive force between the first receiving line and the second receiving line in the axial direction of the logging device in the at least two consecutive measurements at the second measuring point is changed The quantity ^ 1 " and the phase difference variation A PSD are both within the respective predetermined threshold ranges, and the second measurement point is saved as a second homogeneous formation optional point.
如果在步骤 1303和 1304 中经判断没有找到符合上述条件的两个 均质地层可选点, 则返回步骤 1302 , 继续进行随钻测量, 依此类推, 直到找到符合条件的两个均质地层可选点为止。 If it is determined in steps 1303 and 1304 that two homogeneous formation selectable points satisfying the above conditions are not found, then return to step 1302 to continue the measurement while drilling, and so on. Until you find a selection of two homogeneous formations that meet the criteria.
当经由步骤 1303和 1304找到了第一和第二均质地层可选点之后, 在步骤 1305中, 将上述第一和第二均质地层可选点处所测得的所述第 一接收线圏与所述第二接收线圏之间的感应电动势的幅度比的平均值 (即, 在这两个均质地层可选点处所进行的各次测量得到的多个幅度比 的平均值)或均方根和相位差的平均值 (在两个均质地层可选点处所进 行的各次测量得到的多个相位差的平均值) 或均方根分别作为与所测 高阻目的层的地层电阻率相对应的所述测井装置的感应信号的幅度比 基值 "0和相位差基值 PSDQ。  After the first and second homogeneous formation optional points are found via steps 1303 and 1304, in step 1305, the first received line measured at the first and second homogeneous formation optional points An average of amplitude ratios of induced electromotive forces between the 接收 and the second receiving line ( (ie, an average of a plurality of amplitude ratios obtained for each measurement performed at the selectable points of the two homogeneous formations) or The average of the root mean square and phase difference (the average of multiple phase differences obtained from each measurement at two selectable points in the homogeneous formation) or the root mean square as the formation of the layer with the measured high resistance The magnitude of the induced signal of the logging device corresponding to the resistivity is greater than the base value "0" and the phase difference base value PSDQ.
接下来, 在步骤 1306中, 确定并存储所测高阻目的层的地层电阻 率的标准值, 即: 将与所测高阻目的层的地层电阻率相对应的上述幅 度比基值 ^"0和相位差基值 Α¾)θ与各种地层的相应预定本征值进行比 较, 选取与所述幅度比基值和相位差基值最为接近的那一种类型的地 和相位差标准值, 存储所述幅度比标准值和相位差标准值。  Next, in step 1306, the standard value of the formation resistivity of the measured high resistance target layer is determined and stored, that is, the above amplitude ratio base value corresponding to the formation resistivity of the measured high resistance target layer is ^0. And the phase difference base value Α3⁄4) θ is compared with the corresponding predetermined eigenvalues of the various formations, and the type of ground and phase difference standard values closest to the base value and the phase difference base value are selected and stored. The amplitude is greater than the standard value and the phase difference standard value.
可选地, 在步骤 1307中, 根据与所测高阻目的层的地层电阻率对 应的幅度比标准值和相位差标准值来设定所述所测高阻目的层的出层 阔值。 具体而言, 当测井装置靠近低阻边界时, 会造成所述测井装置 的轴向方向的第一接收线圈与第二接收线圏之间的感应电动势的幅度 比和相位差的变化, 测井装置越靠近低阻边界, 所述实测的幅度比相 对于幅度比的标准值的变化量 (即差值) 、 以及所述实测的相位差相 对于相位差的标准值的变化量 (即差值) 就越大, 当该幅度比变化量 和相位差变化量达到或超过预定数值时, 通常认为测井装置的前方出 现低阻地层。 所述预定数值即为本文所述的出层阈值。 需要注意的是, 该出层阈值对于不同的测量地层可以由本领域技术人员根据实际测量 地层的特征及测量情况设定为不同的预定数值, 一般可通过当前所测 地层及前方地层这两种地层的电阻率对比度来加以确定, 优选地, 无 论当前所测地层及前方地层这两种地层的电阻率对比度如何, 均可以 将出层阈值设为幅度比标准值或相位差标准值的 1 %-30%;进一步优选 地, 当所述电阻率对比度为 1 /10时, 可以优选地将出层阔值设为所述 幅度比标准值或相位差标准值的 10%。 上述出层阈值的确定方式以及 数值仅是示例性的, 并不应当构成对本发明保护范围的限制, 本领域 如图所示, 在步骤 1308中, 继续选取下一个测量点, 在下一个测 量点处进行至少两次测量, 计算在该测量点处沿测井装置的轴向方向 的第一接收线圈与第二接收线圈之间的感应电动势的幅度比变化量 ^tt和相位差变化量 Δ PSD。 Optionally, in step 1307, the exit threshold of the measured high resistance target layer is set according to an amplitude ratio standard value and a phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer. Specifically, when the logging device is close to the low resistance boundary, the amplitude ratio and the phase difference of the induced electromotive force between the first receiving coil and the second receiving coil in the axial direction of the logging device are caused. The closer the logging device is to the low resistance boundary, the measured amplitude ratio is the variation (ie, the difference) with respect to the standard value of the amplitude ratio, and the variation of the measured phase difference with respect to the standard value of the phase difference (ie, The larger the difference), when the amplitude ratio change and the phase difference change amount reach or exceed a predetermined value, it is generally considered that a low-resistance formation appears in front of the logging device. The predetermined value is the exit threshold as described herein. It should be noted that the ejecting threshold can be set to different predetermined values according to the characteristics and measurement conditions of the actual measured stratum for the different measured strata by the person skilled in the art, generally through the current measured stratum and the front stratum. The resistivity contrast is determined. Preferably, the exit threshold can be set to an amplitude ratio of 1% of the standard value or the phase difference standard value regardless of the resistivity contrast of the two layers of the current measured formation and the front formation. 30%; Further preferably, when the resistivity contrast is 1 /10, the layer threshold may preferably be set to 10% of the amplitude ratio standard value or phase difference standard value. The manner of determining the above-mentioned layering threshold and the numerical values are merely exemplary, and should not constitute a limitation on the scope of the present invention. As shown, in step 1308, the next measurement point is continued, at least two measurements are taken at the next measurement point, and the first receive coil and the second along the axial direction of the logging device at the measurement point are calculated. The amplitude ratio change amount tt and the phase difference change amount Δ PSD of the induced electromotive force between the receiving coils.
在步骤 1309中,判断步骤 1308中所计算的幅度比变化量 Δ^"和相 位差变化量 A PSD 是否大于出层阈值; 如果大于, 则判定所述测井装 置的前方为低阻地层; 如果不大于, 则存储当前的幅度比变化量 "和 相位差变化量 A PSD,之后判断是否到了预定的第 η个测量点,如果否, 则返回步骤 1308, 继续进行下一测量点的选取及幅度比变化量 和 相位差变化量 A PSD的计算, 如果是到了预定的第 η 个测量点, 则进 入到步骤 1310。 需要注意的是, 此处的 η根据地层的特征及测量的速 度由技术人员根据实际情况来选择, 例如, 如果对于较软的地层 (比 如说濒海地区中的砂岩) , 则 η 的取值可以相对小一些, 而对于较硬 的地层 (比如说页岩) , 则 η 的取值可以相对大一些, 通常, 对于普 通地层而言, η优选地可选为 20-30 , 但本发明绝不限制与此, 其可以 是其他适合的取值。  In step 1309, it is determined whether the amplitude ratio change amount Δ^" and the phase difference change amount A PSD calculated in step 1308 are greater than the exit threshold; if greater, it is determined that the front of the logging device is a low-resistance formation; If not greater than, the current amplitude ratio change amount "and the phase difference change amount A PSD is stored, and then it is determined whether the predetermined nth measurement point has been reached. If not, then return to step 1308 to continue the selection and amplitude of the next measurement point. The calculation of the ratio change amount and the phase difference change amount A PSD , if it is the predetermined nth measurement point, proceeds to step 1310. It should be noted that the η here is selected by the technician according to the actual situation according to the characteristics of the formation and the measured speed. For example, if it is for a softer stratum (such as sandstone in the Bohai area), the value of η It can be relatively small, and for harder formations (such as shale), the value of η can be relatively large. Generally, for ordinary formations, η is preferably 20-30, but the invention is absolutely Without being limited thereto, it may be other suitable values.
在步骤 1310 中, 根据之前所存储的各测量点处的幅度比变化量 和相位差变化量 A PSD来确定幅度比变化趋势和相位差变化趋势; 如果所述变化趋势为从第三个测量点到第 η 个测量点, 所述幅度 比变化量和相位差变化量保持同向递增 (即第 m+ 1 个测量点处的幅度 比变化量和相位差变化量分别比第 m个测量点处的幅度比变化量和相 位差变化量大, 所述 m=l ,2,... ,n-l ) , 则判定所述测井装置的前方为低 阻地层;  In step 1310, the amplitude ratio change trend and the phase difference change trend are determined according to the amplitude ratio change amount and the phase difference change amount A PSD at the respective measurement points stored before; if the change trend is from the third measurement point To the ηth measurement point, the amplitude ratio change amount and the phase difference change amount are kept increasing in the same direction (that is, the amplitude ratio change amount and the phase difference change amount at the m+1 measurement point are respectively higher than the mth measurement point The amplitude ratio change amount and the phase difference change amount are large, and the m=l, 2, . . . , nl) determines that the front of the logging device is a low-resistance formation;
否则如果所述变化趋势总体为同向递增, 则也判定为所述测井装 置的前方为低阻地层; 本文所述的总体同向递增是指: 虽然所述变化 趋势中间有起伏 (也就是说, 在某测量点处的幅度比变化量和相位差 变化量相对于前一测量点处的幅度比变化量和相位差变化量而言有所 减小) , 但是例如至少 70%的测量点保持着同向递增的趋势, 该百分 比也是由技术人员根据实际测量情况来预先设定的, 所述 70%仅为示 例性的, 并不构成对本发明保护范围的限制。  Otherwise, if the trend of change is generally in the same direction, it is also determined that the front of the logging device is a low-resistance formation; the overall same-directional increase described herein means: although there is an ups and downs in the middle of the change trend (ie It is said that the amplitude ratio change amount and the phase difference change amount at a certain measurement point are reduced with respect to the amplitude ratio change amount and the phase difference change amount at the previous measurement point), but for example, at least 70% of the measurement points The trend of increasing in the same direction is maintained, and the percentage is also preset by the technician according to the actual measurement situation. The 70% is merely exemplary and does not constitute a limitation on the scope of protection of the present invention.
如果所述变化趋势既未同向递增, 又未总体同向递增, 则判定所 述测井装置的前方没有出现低阻地层。 If the trend of change is neither increasing in the same direction nor increasing in the same direction, then the decision is made. There is no low-resistance formation in front of the logging device.
根据本发明的另一优选实施例, 在上述步骤 1305中所述的基值确 定过程中, 可以通过磁偶极源并矢格林函数来计算得到第一和第二均 质地层可选点的地层电阻率、 幅度比和相位差。 作为示例, 图 9 - 12 示出了几种示例性的各种测量地层电阻率与幅度比和相位差的本征值 对照表, 该本征值对照表中的相应物理量通过磁偶极源并矢格林函数 来计算得到。 其中, 图 9 示出了根据本发明优选实施例的测井装置天 线对 T2-R1 -R2在 2MHz的发射频率下的各种测量地层电阻率与幅度比 和相位差转换的本征值的对照表; 图 10示出了根据本发明优选实施例 的测井装置天线对 T2-R1 -R2在 400kHz的发射频率下的各种测量地层 电阻率与幅度比和相位差转换的本征值的对照表; 图 1 1 示出了根据本 发明优选实施例的测井装置天线对 T 1 -R1 -R2在 2MHz的发射频率下的 各种测量地层电阻率与幅度比和相位差转换的本征值的对照表; 图 12 示出了根据本发明优选实施例的测井装置天线对 T1 -R1 -R2在 400kHz 的发射频率下的各种测量地层电阻率与幅度比和相位差转换的本征值 的对照表。  According to another preferred embodiment of the present invention, in the base value determining process described in the above step 1305, the formation of the first and second homogeneous layer selectable points may be calculated by the magnetic dipole source dyadic Green's function. Resistivity, amplitude ratio, and phase difference. By way of example, Figures 9-12 illustrate several exemplary eigenvalue comparison tables for measuring formation resistivity versus amplitude ratio and phase difference, the corresponding physical quantities in the eigenvalue comparison table passing through the magnetic dipole source and The vector green function is calculated. 9 is a comparison of various measured formation resistivity and amplitude ratios and phase difference converted eigenvalues of the logging device antenna for T2-R1 -R2 at a transmission frequency of 2 MHz according to a preferred embodiment of the present invention. Figure 10 shows a comparison of various measured formation resistivity and amplitude ratios and phase difference converted eigenvalues of a logging device antenna for T2-R1 - R2 at a transmission frequency of 400 kHz in accordance with a preferred embodiment of the present invention. Figure 1 1 shows various measured formation resistivity and amplitude ratios and phase difference converted eigenvalues of a logging device antenna for T 1 -R1 -R2 at a transmission frequency of 2 MHz in accordance with a preferred embodiment of the present invention. Figure 12 shows the eigenvalues of various measured formation resistivity and amplitude ratios and phase difference conversions of the logging device antenna for T1 - R1 - R2 at a transmission frequency of 400 kHz in accordance with a preferred embodiment of the present invention. Comparison table.
此外, 根据本发明的再一优选实施例, 所述测井方法还优选地包 括采用索末菲尔德积分计算前方低阻地层到测井装置 (例如根据本发 明的电磁波传播电阻率前向探测装置) 的距离。  Moreover, in accordance with still another preferred embodiment of the present invention, the logging method preferably further comprises calculating a front low resistance formation to a logging device using a Sommerfeld integral (eg, an electromagnetic wave propagation resistivity forward detecting device in accordance with the present invention) the distance.
本申请的图 2 示出了优选地采用根据本发明优选实施例的电磁波 传播电阻率前向探测装置进行前向探测的测井方法所用到的二层地层 模型图。  Figure 2 of the present application shows a two-layer formation model diagram preferably used in a logging method for forward detection of an electromagnetic wave propagation resistivity forward detecting device in accordance with a preferred embodiment of the present invention.
如图 2中所示, 各附图标记分别表示: 地层 1 ; 2 : 地层 2; 3 : 地层 1和地层 2间的层界面; 4: 电磁波传播电阻率前向探测装置的心 轴线; 5 : 电磁波传播电阻率前向探测装置的测量点; 6: 电磁波传播 电阻率前向探测装置的测量点到地层 1和地层 2间的层界面 3的距离; 7: 安装角为零的接收天线 R1 ; 8: 安装角优选为零度的接收天线 R2; 9: 安装角优选为 45° 的接收天线 R3 ; 10: 安装角优选为 -45° 的接 收天线 R4; 1 1、 安装角优选为零度的发射天线 Tl。 根据该二层地层模 型, 所述电磁波传播电阻率前向探测装置被设置在地层 1 中并且垂直 于地层 1 和地层 2的界面, 通过改变地层界面 3到装置中心点的距离 即可获得在不同电阻率对比度的地层中幅度衰减和相位移的变化。 图 3至图 8示出的是根据本发明优选实施例的电磁波传播电阻率 前向探测装置的不同发射-接收天线对在采用不同频率时在不同的电 阻率对比度地层的幅度衰减响应或相位移响应随地层界面位置的变 化关系图。图 3-图 8中的横坐标表示从地层界面 3到装置中心点的距 离, 纵坐标表示线圈系在二层地层中与在以地层 1的电参数为电阻率 的均质地层中的响应的差值。 As shown in Fig. 2, each reference numeral denotes: formation 1; 2: formation 2; 3: layer interface between formation 1 and formation 2; 4: electromagnetic wave propagation resistivity forward detection device core axis; 5: Electromagnetic wave propagation resistivity measurement point of the forward detecting device; 6: Electromagnetic wave propagation resistivity The distance from the measuring point of the forward detecting device to the layer interface 3 between the ground layer 1 and the ground layer 2; 7: The receiving antenna R1 with a mounting angle of zero; 8: receiving antenna R2 with a mounting angle of preferably zero degrees; 9: receiving antenna R3 with a mounting angle of preferably 45°; 10: receiving antenna R4 with a mounting angle of preferably -45°; 1 1 , a transmitting antenna with a mounting angle of preferably zero Tl. According to the two-layer formation model, the electromagnetic wave propagation resistivity forward detecting device is disposed in the formation 1 and perpendicular to the interface of the formation 1 and the formation 2, and can be obtained by changing the distance between the formation interface 3 and the center point of the device. Amplitude attenuation and phase shift changes in the formation with resistivity contrast. 3 to 8 illustrate amplitude attenuation responses or phase shifts of different transmit-receive antenna pairs in different resistivity contrast formations when different frequencies are employed, in accordance with a preferred embodiment of the present invention. Respond to changes in the position of the interface with the ground plane. The abscissas in Figures 3-8 represent the distance from the formation interface 3 to the center point of the device, and the ordinate indicates the response of the coil system in the two formations and in the homogeneous formation in which the electrical parameters of the formation 1 are resistivity. Difference.
假设根据本发明优选实施例的电磁波传播电阻率前向探测装置的 幅度衰减阔值为 0.02dB、相位移的阈值为 0. Γ (如图 3-图 8中的横线 所示), 则由图 3至图 8可得到该探测装置中的各天线对在不同电阻 率对比度地层中的垂向探测深度。  It is assumed that the amplitude-attenuation threshold of the electromagnetic wave propagation resistivity forward detecting device according to the preferred embodiment of the present invention is 0.02 dB, and the phase shift threshold is 0. Γ (shown by the horizontal line in FIGS. 3-8) 3 to 8 can obtain the vertical depth of detection of each pair of antennas in the detection device in different resistivity contrast formations.
例如, 在 10/1 电阻率对比度地层中, 若发射-接收天线对的频率为 2MHz, 则 16/22in. (即英寸 )天线对的幅度衰减和相位移的垂向探测 深度分别为 41 in.和 26 in., 32/38ιη.天线对的幅度衰减和相位移的垂 向探测深度分别为 56 in.和 37 in. ; 如果发射-接收天线对的频率为 400kHz, 则 16/22in.天线对的幅度衰减和相位移的垂向探测深度分别 为 43 in.和 35 in. , 32/38in.天线对的幅度衰减和相位移的垂向探测深 度分别为 67 in.和 48 in.。  For example, in a 10/1 resistivity contrast formation, if the frequency of the transmit-receive antenna pair is 2 MHz, the amplitude attenuation of the 16/22 in. (ie inches) antenna pair and the vertical depth of the phase shift are 41 in. And 26 in., 32/38ιη. The amplitude attenuation of the antenna pair and the vertical depth of the phase shift are 56 in. and 37 in. respectively; if the frequency of the transmit-receive antenna pair is 400 kHz, the 16/22 in. antenna pair The amplitudes of the amplitude attenuation and phase shift are 43 in. and 35 in., respectively, and the 32/38 in. antenna pair amplitude attenuation and phase displacement vertical detection depth are 67 in. and 48 in., respectively.
在 50/1 电阻率对比度地层中, 若所述频率取 2MHz, 则 16/22in. 天线对的幅度衰减和相位移的垂向探测深度分别为 55 in.和 35 in.、 32/38in.天线对的幅度衰减和相位移的垂向探测深度分别为 77 in.和 46 in. ; 若所述频率取 400kHz, 则 16/22in.天线对的幅度衰减和相位 移的垂向^!罙测深度分别为 49 in.和 44 in. , 32/38in.天线对的幅度衰减 和相位移的垂向探测深度分别为 82 in.和 62 ιη.。  In the 50/1 resistivity contrast formation, if the frequency is 2MHz, the amplitude attenuation of the 16/22in. antenna pair and the vertical depth of the phase shift are 55 in. and 35 in., 32/38 in. The vertical attenuation depths of the amplitude attenuation and phase shift are 77 in. and 46 in. respectively; if the frequency is 400 kHz, the amplitude attenuation of the antenna pair and the vertical displacement of the phase shift ^! The amplitudes of amplitude attenuation and phase shift of the antenna pairs of 49 in. and 44 in., 32/38 in. respectively are 82 in. and 62 ηη.
在 200/1 电阻率对比度地层中, 若所述频率取 2MHz, 则 16/22in. 天线对的幅度衰减和相位移的垂向探测深度分别为 61 in.和 43 in.、 32/38in.天线对的幅度衰减和相位移的垂向探测深度分别为 92 in.和 57 in. ; 若所述频率取 400kHz, 则 16/22in.天线对的幅度衰减和相位 移的垂向探测深度分别为 50 in.和 47 in. , 32/38in.天线对的幅度衰减 和相位移的垂向探测深度分别为 87 in.和 71 in.。  In a 200/1 resistivity contrast formation, if the frequency is 2 MHz, the amplitude attenuation of the 16/22 in. antenna pair and the vertical depth of phase shift are 61 in. and 43 in., 32/38 in. antenna, respectively. The vertical depths of amplitude attenuation and phase shift are 92 in. and 57 in. respectively; if the frequency is 400 kHz, the amplitude attenuation of the 16/22 in. antenna pair and the vertical depth of phase shift are 50 respectively. In. and 47 in. , 32/38 in. The amplitude attenuation of the antenna pair and the vertical depth of phase shift are 87 in. and 71 in., respectively.
由图 3至图 8 可以看出, 随着地层电阻率对比度的增加, 幅度衰 减响应或相位移响应随地层界面位置的变化更加平緩。 随着地层电阻 率对比度和天线对线圏距的增加, 所述探测装置的垂向探测深度增大。 在相同电阻率对比度地层中, 同一天线对幅度衰减曲线的垂向探测深 度大于相位移曲线的垂向探测深度。 It can be seen from Fig. 3 to Fig. 8 that as the resistivity contrast of the formation increases, the amplitude attenuation response or the phase displacement response changes more gently with the position of the formation interface. As the formation resistivity contrast and the antenna pitch increase, the vertical depth of the detection device increases. In the same resistivity contrast formation, the vertical detection depth of the amplitude attenuation curve of the same antenna is greater than the vertical detection depth of the phase displacement curve.
在钻井装置向前钻进的过程中, 通过根据本发明的设置在钻井装 置中的所述随钻测井装置实时测量上述幅度衰减或相位移信号的变化 可以确定地层界面或油水界面的存在, 从而控制钻具穿行在油藏的最 佳位置。 如果在钻井装置向前钻进的过程中所述随钻测井装置没有出 现上述幅度衰减或相位移信号的变化, 也就是随钻测井装置的幅度衰 减或相位移信号的读数为定值, 则表示无低阻地层存在。 若在钻井装 置向前钻进的过程中上述幅度衰减或相位移信号的读数发生改变, 则 表示钻井装置前方出现了低阻地层, 需及时调整井眼轨迹以避免钻入 低阻地层, 从而使钻井装置始终位于高阻含油目的层段, 进而实现地 层界面的钻前预测和精确地质导向。  The presence of the formation interface or the oil-water interface may be determined by measuring the amplitude attenuation or the phase shift signal in real time by the logging while drilling device disposed in the drilling device according to the present invention during the forward drilling of the drilling device. This controls the drill to travel through the best position in the reservoir. If the LWD tool does not exhibit the above-mentioned amplitude attenuation or phase shift signal change during the drilling of the drilling device, that is, the amplitude attenuation of the LWD device or the reading of the phase shift signal is constant. This means that there is no low-resistance formation. If the amplitude attenuation or phase shift signal reading changes during the forward drilling of the drilling unit, it means that there is a low-resistance formation in front of the drilling unit, and the wellbore trajectory needs to be adjusted in time to avoid drilling into the low-resistance formation, thus The drilling unit is always located in the high-resistance oil-bearing purpose interval, thereby achieving pre-drilling prediction and precise geosteering of the formation interface.
需要指出的是, 本发明虽然参照石油钻井来描述了优选实施例, 但是本发明的测井装置及测井方法并不仅限于石油钻井领域, 还广泛 地适用于采煤、 采矿等其他钻井行业中。  It should be noted that although the present invention has described preferred embodiments with reference to oil drilling, the logging apparatus and logging method of the present invention are not limited to the field of oil drilling, but are also widely applicable to other drilling industries such as coal mining and mining. .
下面, 本说明书将进一步描述用于实现根据本发明优选实施例的 所述测井方法的数据处理设备。  Hereinafter, the present specification will further describe a data processing apparatus for implementing the logging method according to a preferred embodiment of the present invention.
如图 14所示, 根据本发明的数据处理设备优选地包括: 第一、 第 二测量点选取装置 1400、 第一幅度比变化量和相位差变化量计算装置 1401、 第二幅度比变化量和相位差变化量计算装置 1402、 第一均质地 层可选点判定装置 1403、 第二均质地层可选点判定装置 1404、 存储装 置 1405、 基值确定装置 1406、 标准值确定装置 1407、 出层阈值设定装 置 1408、第三 -第 n测量点选取及计算装置 1409以及低阻地层判定装 置 1410。  As shown in FIG. 14, the data processing apparatus according to the present invention preferably includes: first and second measurement point selecting means 1400, first amplitude ratio change amount and phase difference change amount calculating means 1401, second amplitude ratio change amount and Phase difference variation calculation device 1402, first homogeneous formation optional point determination device 1403, second homogeneous formation optional point determination device 1404, storage device 1405, base value determination device 1406, standard value determination device 1407, and egress layer Threshold setting means 1408, third-nth measurement point selection and calculation means 1409 and low resistance formation determination means 1410.
其中, 所述第一、 第二测量点选取装置 1400选取两个连续测量点 (即第一测量点和第二测量点) , 并指示测井装置在每个所选取的测 量点处进行至少两次连续测量。  The first and second measurement point selection devices 1400 select two consecutive measurement points (ie, a first measurement point and a second measurement point), and instruct the logging device to perform at least two at each selected measurement point. Sub-continuous measurement.
所述第一、 第二测量点选取装置 1400分别耦合到所述第一幅度比 变化量和相位差变化量计算装置 1401和第二幅度比变化量和相位差变 化量计算装置 1402。  The first and second measurement point selecting means 1400 are coupled to the first amplitude ratio change amount and phase difference change amount calculating means 1401 and the second amplitude ratio change amount and phase difference change amount calculating means 1402, respectively.
所述第一幅度比变化量和相位差变化量计算装置 1401用于计算在 所述第一、 第二测量点选取装置 1400所选取的第一测量点处、 在所述 至少两次连续测量中沿测井装置轴向方向的第一接收线圈与第二接收 线圈之间的感应电动势的幅度比变化量 A^t和相位差变化量 A PSD; 所述第二幅度比变化量和相位差变化量计算装置 1402用于计算在 所述第一、 第二测量点选取装置 1400所选取的第二测量点处、 在所述 至少两次连续测量中沿测井装置轴向方向的第一接收线圏与第二接收 线圏之间的感应电动势的幅度比变化量 Δ ί"和相位差变化量 A PSD; 所述第一均质地层可选点判定装置 1403耦合至所述第一幅度比变 化量和相位差变化量计算装置 1401 , 且用于判断在第一测量点处、 沿 测井装置轴向方向的第一接收线圏与第二接收线圏之间的感应电动势 的幅度比变化量 和相位差变化量 A PSD 是否在其各自的预定阚值 范围内, 如果是, 则将该第一测量点作为第一均质地层可选点保存在 存储装置 1405中。如果否,则指示所述第一、第二测量点选取装置 1400 重新选取测量点。 优选地, 上述预定幅度比变化量阈值范围可以为 0-0.03dB或其他预定范围,预定相位差变化量阈值范围为 0°-0.1°或其他 预定范围。 The first amplitude ratio change amount and phase difference change amount calculation means 1401 is configured to calculate at the first measurement point selected by the first and second measurement point selection means 1400, An amplitude ratio change amount A^t and a phase difference change amount A PSD of the induced electromotive force between the first receiving coil and the second receiving coil in the axial direction of the logging device in at least two consecutive measurements; the second amplitude ratio The variation and phase difference variation calculation device 1402 is configured to calculate the axial direction along the logging device at the second measurement point selected by the first and second measurement point selection devices 1400 in the at least two consecutive measurements An amplitude ratio change amount Δί" of the induced electromotive force between the first receiving line 圏 and the second receiving line 方向 and a phase difference change amount A PSD; the first homogeneous formation selectable point determining device 1403 is coupled to the The first amplitude ratio change amount and phase difference change amount calculating means 1401 is configured to determine the sensing between the first receiving line 圏 and the second receiving line 轴向 in the axial direction of the logging device at the first measuring point The amplitude ratio change amount and the phase difference change amount A PSD of the electromotive force are within their respective predetermined threshold values, and if so, the first measurement point is stored as the first homogeneous formation optional point in the storage device 1405. If no, the indication office The first and second measuring point selecting means 1400 reselect the measuring point. Preferably, the predetermined amplitude ratio change amount threshold value range may be 0-0.03 dB or other predetermined range, and the predetermined phase difference change amount threshold value range is 0°-0.1 ° or other predetermined range.
所述第二均质地层可选点判定装置 1404耦合至所述第二幅度比变 化量和相位差变化量计算装置 1402 , 且用于判断在第二测量点处、 沿 测井装置轴向方向的第一接收线圏与第二接收线圈之间的感应电动势 的幅度比变化量 和相位差变化量 A PSD 是否在其各自的预定阈值 范围内, 如果是, 则将该第二测量点作为第二均质地层可选点保存在 存储装置 1405中。如果否,则指示所述第一、第二测量点选取装置 1400 重新选取测量点。  The second homogeneous formation selectable point determining device 1404 is coupled to the second amplitude ratio change amount and phase difference change amount calculating means 1402, and is configured to determine the axial direction of the logging device at the second measuring point Whether the amplitude ratio change amount and the phase difference change amount A PSD of the induced electromotive force between the first receiving line 圏 and the second receiving coil are within their respective predetermined threshold ranges, and if so, the second measuring point is taken as the first The optional points of the two homogeneous formations are stored in the storage device 1405. If not, the first and second measurement point selection means 1400 are instructed to reselect the measurement point.
所述基值确定装置 1406耦合至存储装置 1405 ,且用于确定与所测 高阻目的层的地层电阻率相对应的所述测井装置的感应信号的幅度比 基值 0和相位差基值 ¾£»o。 根据优选实施例, 基值确定装置 1406将 存储装置 1405中所存储的上述第一和第二均质地层可选点处所测得的 第一接收线圈与第二接收线圏之间的感应电动势的幅度比的平均值 (在 这两个均质地层可选点处所进行的各次测量得到的多个幅度比的平均 值)或均方根和相位差的平均值 (在两个均质地层可选点处所进行的各 次测量得到的多个相位差的平均值) 或均方根分别作为与所测高阻目 的层的地层电阻率对应的幅度比基值 ^"0和相位差基值 PSDQ。  The base value determining device 1406 is coupled to the storage device 1405 and configured to determine an amplitude ratio of the sensing signal of the logging device corresponding to the formation resistivity of the measured high resistance target layer to a base value of 0 and a phase difference base value 3⁄4£»o. According to a preferred embodiment, the base value determining means 1406 senses the induced electromotive force between the first receiving coil and the second receiving coil at the first and second homogeneous formation selectable points stored in the storage means 1405. The average of the amplitude ratios (average of multiple amplitude ratios for each measurement made at the optional points of the two homogeneous formations) or the average of the root mean square and phase difference (in two homogeneous formations) The average value of the plurality of phase differences obtained by each measurement at the optional point or the root mean square is respectively used as the amplitude ratio base value ^"0 and the phase difference base value corresponding to the formation resistivity of the measured high resistance target layer. PSDQ.
优选地, 所述基值确定装置 1406通过磁偶极源并矢格林函数来计 算得到所述第一和第二均质地层可选点的地层电阻率、 幅度比和相位 差。 要指出的是, 所述基值确定装置 1406还可以釆用其他已有函数或 算法来计算得到所述第一和第二均质地层可选点的地层电阻率、 幅度 比和相位差。 Preferably, the base value determining means 1406 is calculated by a magnetic dipole source dyadic Green's function The formation resistivity, the amplitude ratio and the phase difference of the selectable points of the first and second homogeneous formations are calculated. It is to be noted that the base value determining means 1406 may also use other existing functions or algorithms to calculate the formation resistivity, amplitude ratio and phase difference of the selectable points of the first and second homogeneous formations.
所述标准值确定装置 1407耦合至所述基值确定装置 1406和存储 装置 1405 ,并用于确定并存储所测高阻目的层的地层电阻率的标准值。 根据优选实施例, 所述标准值确定装置 1407用于将与所测高阻目的层 的地层电阻率对应的上述幅度比基值 和相位差基值 与各种地 层的相应预定本征值进行比较, 选取与所述幅度比基值和相位差基值 最为接近的那一种类型的地层的本征值作为与所测高阻目的层的地层 电阻率对应的幅度比标准值和相位差标准值, 并将所述幅度比标准值 和相位差标准值存储在存储装置 1405中。  The standard value determining means 1407 is coupled to the base value determining means 1406 and the storage means 1405 and is used to determine and store a standard value of the formation resistivity of the measured high resistance target layer. According to a preferred embodiment, the standard value determining means 1407 is adapted to compare the amplitude ratio base value and phase difference base value corresponding to the formation resistivity of the measured high resistance target layer with corresponding predetermined eigenvalues of various formations. Selecting an eigenvalue of the type of the layer closest to the base value and the phase difference base value as the amplitude ratio standard value and phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer And storing the amplitude in the storage device 1405 in comparison with the standard value and the phase difference standard value.
所述出层阔值设定装置 1408耦合至所述标准值确定装置 1407和 存储装置 1405 , 并用于设定所测高阻目的层的出层阈值。 根据优选实 施例, 所述出层阈值设定装置 1408根据与所测高阻目的层的地层电阻 率对应的幅度比标准值和相位差标准值来设定所述所测高阻目的层的 出层阔值, 之后优选地将所述出层阈值存储在所述存储装置 1405中。  The exit threshold setting means 1408 is coupled to the standard value determining means 1407 and the storage means 1405 and is used to set the exit threshold of the measured high resistance target layer. According to a preferred embodiment, the exit layer threshold setting means 1408 sets the output of the measured high resistance target layer according to an amplitude ratio standard value and a phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer. The layer threshold is then preferably stored in the storage device 1405.
具体而言, 当测井装置靠近低阻边界时, 会造成所述测井装置的 轴向方向的第一接收线圏与第二接收线圏之间的感应电动势的幅度比 和相位差的变化, 测井装置越靠近低阻边界, 所述实测的幅度比相对 于幅度比的标准值的变化量 (即差值) 、 以及所述实测的相位差相对 于相位差的标准值的变化量 (即差值) 就越大, 当该幅度比变化量和 相位差变化量达到或超过预定数值时, 通常认为测井装置的前方出现 低阻地层。 所述预定数值即为本文所述的出层阈值。 如前所述, 该出 层阈值对于不同的测量地层可以由本领域技术人员根据实际测量地层 的特征及测量情况设定为不同的预定数值, 一般可通过当前所测地层 及前方地层这两种地层的电阻率对比度来加以确定, 优选地, 无论当 前所测地层及前方地层这两种地层的电阻率对比度如何, 均可以将出 层阈值设为幅度比标准值或相位差标准值的 1 %-30%; 进一步优选地, 当所述电阻率对比度为 1 /10时, 可以优选地将出层阈值设为所述幅度 比标准值或相位差标准值的 10%。 上述出层阈值的确定方式以及数值 仅是示例性的, 并不应当构成对本发明保护范围的限制, 本领域技术 人员可以根据实际情况通过其他方式选择合适的数值。 Specifically, when the logging device is close to the low resistance boundary, the amplitude ratio and the phase difference of the induced electromotive force between the first receiving line 圏 and the second receiving line 轴向 in the axial direction of the logging device are caused. The closer the logging device is to the low resistance boundary, the measured amplitude ratio is the variation amount (ie, the difference) with respect to the standard value of the amplitude ratio, and the variation of the measured phase difference with respect to the standard value of the phase difference ( The larger the difference, the greater the resistance, the change in the amount of change and the phase difference to or above a predetermined value is generally considered to occur in the front of the logging device. The predetermined value is the exit threshold as described herein. As described above, the threshold of the egress layer can be set to different predetermined values according to the characteristics and measurement conditions of the actual measurement stratum for the different measurement strata by the person skilled in the art, generally through the two layers of the current measured stratum and the front stratum. The resistivity contrast is determined. Preferably, the exit threshold can be set to an amplitude ratio of 1% of the standard value or the phase difference standard value regardless of the resistivity contrast of the two layers of the current measured formation and the front formation. 30%; Further preferably, when the resistivity contrast is 1 /10, the layer threshold may preferably be set to 10% of the amplitude ratio standard value or phase difference standard value. The manner of determining the above-mentioned layering threshold and the numerical values are merely exemplary, and should not constitute a limitation on the scope of the present invention. Personnel can choose the appropriate value by other means according to the actual situation.
所述第三-第 n测量点选取及计算装置 1409用于继续选取下一个 测量点, 在下一个测量点处进行至少两次测量, 计算在该测量点处沿 测井装置的轴向方向的第一接收线圏与第二接收线圏之间的感应电动 势的幅度比变化量 和相位差变化量△ PSD。  The third-nth measurement point selection and calculation device 1409 is configured to continue to select the next measurement point, perform at least two measurements at the next measurement point, and calculate the first direction along the axial direction of the logging device at the measurement point. The amplitude ratio change amount and the phase difference change amount Δ PSD of the induced electromotive force between a receiving line 圏 and the second receiving line 。.
所述低阻地层判定装置 1410分别耦合至存储装置 1405、出层阈值 设定装置 1408以及所述第三 -第 n测量点选取及计算装置 1409。  The low resistance formation determining means 1410 is coupled to the storage means 1405, the exit threshold setting means 1408 and the third - nth measuring point selecting and calculating means 1409, respectively.
根据优选实施例, 所述低阻地层判定装置 1410包括出层阈值判定 单元 14101 , 其用于判断所述第三 -第 n测量点选取及计算装置 1409 中所计算的当前测量点的幅度比变化量^ 和相位差变化量 A PSD 是 否大于出层阈值; 如果大于, 则判定所述测井装置的前方为低阻地层; 如果不大于,则优选地将当前测量点的幅度比变化量 和相位差变化 量 A PSD存储在存储装置 1405中。  According to a preferred embodiment, the low-resistance formation determining device 1410 includes a layering threshold determining unit 14101 for determining a change in the amplitude ratio of the current measuring point calculated in the third-nth measuring point selection and computing device 1409. Whether the quantity ^ and the phase difference change amount A PSD is greater than the exit threshold; if it is greater, it is determined that the front of the logging device is a low-resistance formation; if not, the amplitude ratio of the current measurement point is preferably changed and phase The difference variation A PSD is stored in the storage device 1405.
根据另一优选实施例, 所述低阻地层判定装置 1410还包括测量点 数目判定单元 14102和幅度比及相位差变化趋势判定单元 14103。  According to another preferred embodiment, the low-resistance formation determining means 1410 further includes a measuring point number determining unit 14102 and an amplitude ratio and phase difference changing tendency determining unit 14103.
所述测量点数目判定单元 14102 用于在所述出层阈值判定单元 14101判断当前测量点的幅度比变化量 和相位差变化量 A PSD不大 于出层阈值时, 判断当前测量点是否已达到预定的第 n 个测量点, 如 果否, 则指示所述第三-第 n测量点选取及计算装置 1409继续进行下 一测量点的选取及幅度比变化量 Δ^"和相位差变化量 A PSD的计算;反 之, 如果当前测量点为预定的第 η 个测量点, 则指示幅度比及相位差 变化趋势确定单元 14103来根据之前所存储的各测量点(即第 3、4、5... η 个测量点)处的幅度比变化量 Δ^"和相位差变化量 A PSD来确定幅度比 变化趋势和相位差变化趋势。  The measurement point number determining unit 14102 is configured to determine whether the current measurement point has reached the predetermined time when the out-of-layer threshold value determining unit 14101 determines that the amplitude ratio change amount and the phase difference change amount A PSD of the current measurement point are not greater than the exit threshold value. The nth measurement point, if not, instructs the third-nth measurement point selection and calculation device 1409 to continue the selection of the next measurement point and the amplitude ratio change amount Δ^" and the phase difference variation A PSD If the current measurement point is the predetermined nth measurement point, the indication amplitude ratio and phase difference change trend determining unit 14103 is based on the previously stored measurement points (ie, 3, 4, 5... η The amplitude ratio change amount Δ^" and the phase difference change amount A PSD at the measurement point) determine the amplitude ratio change tendency and the phase difference change tendency.
如前所述, 此处的 η 根据地层的特征及测量的速度由技术人员根 据实际情况来选择, 例如, 如果对于较软的地层 (比如说瀕海地区的 砂岩) , 则 η 的取值可以相对小一些, 而对于较硬的地层 (比如说页 岩) , 则 η的取值可以相对大一些, 通常, 对于普通地层而言, η优选 地可选为 20-30, 但本发明绝不限制与此, 其可以是其他适合的取值。  As mentioned above, η here is selected by the technician according to the actual conditions of the formation according to the characteristics of the formation and the measured speed. For example, if for a softer formation (such as sandstone in the Bohai area), the value of η can be Relatively small, and for harder formations (such as shale), the value of η can be relatively large. Generally, for ordinary formations, η is preferably 20-30, but the present invention never Limits to this, it can be other suitable values.
根据再一优选实施例, 所述低阻地层判定装置 1410还包括同向递 增变化趋势判定单元 14104 ,所述同向递增变化趋势判定单元 14104用 于判断由所述幅度比及相位差变化趋势确定单元 14103 确定的所述变 化趋势是否为从第三个测量点到第 n 个测量点, 所述幅度比变化量和 相位差变化量保持同向递增 (即第 m+ 1 个测量点处的幅度比变化量和 相位差变化量分别比第 m个测量点处的幅度比变化量和相位差变化量 大, 所述 m=l ,2,... ,n-l ) , 如果是, 则判定所述测井装置的前方为低阻 地层。 According to still another preferred embodiment, the low-resistance formation determining device 1410 further includes a co-directional incremental change trend determining unit 14104, wherein the co-directional incremental change trend determining unit 14104 is configured to determine that the amplitude ratio and the phase difference change trend are determined. The change determined by unit 14103 Whether the trend is from the third measurement point to the nth measurement point, the amplitude ratio change amount and the phase difference change amount keep increasing in the same direction (that is, the amplitude ratio change amount and phase difference change at the m+1 measurement point) The amount is larger than the amplitude ratio change amount and the phase difference change amount at the mth measurement point, respectively, the m=l, 2, . . . , nl), and if yes, the front of the logging device is determined to be low Resist the formation.
根据又一优选实施例, 所述低阻地层判定装置 1410还包括总体同 向递增变化趋势判定单元 14105,其用于在判定单元 14104的判定结果 为否的时候判断所述变化趋势是否总体为同向递增, 如果是, 则判定 为所述测井装置的前方为低阻地层; 如果否, 则判定所述测井装置的 前方没有出现低阻地层。 如前所迷, 此处的总体同向递增是指: 虽然 所迷变化趋势中间有起伏 (也就是说, 在某测量点处的幅度比变化量 和相位差变化量相对于前一测量点处的幅度比变化量和相位差变化量 而言有所减小) , 但是例如至少 70%的测量点保持着同向递增的趋势, 该百分比也是由技术人员根据实际测量情况来预先设定的, 所述 70% 仅为示例性的, 并不构成对本发明保护范围的限制。  According to still another preferred embodiment, the low-resistance formation determining device 1410 further includes an overall in-situ incremental change trend determining unit 14105, configured to determine whether the change trend is the same when the determination result of the determining unit 14104 is negative. The direction is incremented, and if so, it is determined that the front of the logging device is a low resistance formation; if not, it is determined that no low resistance formation is present in front of the logging device. As previously mentioned, the overall in-situ increment here means: although there is an ups and downs in the middle of the trend (that is, the amplitude ratio change and the phase difference change at a certain measurement point are relative to the previous measurement point). The amplitude is smaller than the amount of change and the amount of phase difference change), but for example, at least 70% of the measurement points maintain a trend of increasing in the same direction, which is also preset by the technician based on the actual measurement. The 70% is merely exemplary and does not constitute a limitation of the scope of the present invention.
请注意, 可以以硬件、 软件、 固件或其组合来实现本优选实施例。 在 (一个或多个) 各种实施例中, 以存储在存储器中并由适当的指令 执行系统执行的软件或固件来实现设备组件。 如果以硬件实现, 如在 某些实施例中, 则可以用在本领域中全部众所周知的任何以下技术或 其组合来实现设备组件: 具有用于对数据信号实现逻辑功能的逻辑门 的 (一个或多个) 离散逻辑电路、 具有适当组合逻辑门的专用集成电 路 (ASIC ) 、 (一个或多个) 可编程门阵列 (PGA ) 、 现场可编程门 阵列 ( FPGA ) 等。  Please note that the preferred embodiment can be implemented in hardware, software, firmware or a combination thereof. In various embodiments(s), the device components are implemented in software or firmware stored in a memory and executed by a suitable instruction execution system. If implemented in hardware, as in some embodiments, the device components can be implemented with any of the following techniques or combinations thereof well known in the art: having a logic gate for implementing logic functions on data signals (one or Multiple) discrete logic circuits, application specific integrated circuits (ASICs) with appropriate combinational logic gates, programmable gate array(s) (PGA), field programmable gate arrays (FPGAs), and more.
软件组件可以包括用于实现逻辑功能的可执行指令的有序列表, 可以体现在任何计算机可读介质中以供指令执行系统、 装置或设备使 用或与之相结合地使用, 所述指令执行系统、 装置或设备诸如为基于 计算机的系统、 包含处理器的系统、 或能够从指令执行系统、 装置或 设备获取指令并执行该指令的其它系统。 另外, 本公开的范围包括在 在硬件或软件构造的介质中体现的逻辑中体现一个或多个实施例的功 能。  A software component can include an ordered list of executable instructions for implementing logical functions, which can be embodied in any computer readable medium for use by or in connection with an instruction execution system, apparatus, or device, the instruction execution system A device or device, such as a computer-based system, a system containing a processor, or other system capable of acquiring instructions from an instruction execution system, apparatus, or device and executing the instructions. Further, the scope of the present disclosure includes the functionality of one or more embodiments embodied in logic embodied in a hardware or software constructed medium.
已经出于图示和说明的目的提出了本公开的实施例的前述公幵。 公开, 本文所述的实施例的许多变更和修改对于本领域的普通技术人 员来说将是显然的。 请注意, 上述示例并不意图是限制性的。 还可以 预期可以包括许多上述特征的装置、 方法和设备的附加实施例。 在研 究附图和详细说明之后, 本公开的其它装置、 方法、 设备、 特征和优 点对于本领域的技术人员来说更加显而易见。 意图在于将所有此类其 它装置、 方法、 设备、 特征和优点包括在本发明的保护范围内。 解, 否则诸如 "能够" 、 "可" 、 "可能,, 或 "可以" 之类的条件语 言一般旨在传达的是某些实施例可以包括但不必须包括某些特征、 元 件和 /或步骤。 因此, 此类条件语言通常并不旨在暗示以任何方式要求 一个或多个实施例必须包括特征、 元件和 /或步骤。 The foregoing disclosure of the embodiments of the present disclosure has been presented for purposes of illustration and description. Many variations and modifications of the embodiments described herein will be apparent to those skilled in the art. Please note that the above examples are not intended to be limiting. Additional embodiments of devices, methods and apparatus that can include many of the above features are also contemplated. Other devices, methods, devices, features, and advantages of the present disclosure will be apparent to those skilled in the <RTIgt; All such other devices, methods, devices, features, and advantages are intended to be included within the scope of the present invention. Solution, otherwise conditional languages such as "can", "may", "may," or "may" are generally intended to convey that certain embodiments may include, but do not necessarily include certain features, components, and/or steps. Therefore, such conditional language is not intended to imply that any one or more embodiments are required to include features, elements and/or steps.
应将流程图中的任何处理说明或方框理解为表示包括用于实现该 处理中的特定逻辑功能或步骤的一个或多个可执行指令的代码部分、 , 其中, 可以不按所 ^或所^ "论的顺序来执行功能: ^括基本上同 时地或按照相反顺序, 其取决于所涉及的功能, 如本公开的领域中的 理性技术人员将理解的那样。  Any processing description or block in the flowcharts should be understood to represent a portion of the code that includes one or more executable instructions for implementing a particular logical function or step in the process, in which the The order of the arguments is to perform the functions: Included substantially simultaneously or in reverse order, depending on the function involved, as will be understood by a skilled person in the field of the present disclosure.

Claims

权 利 要 求 Rights request
1. 一种测井方法, 其包括: A logging method comprising:
( a ) 均质测量点选取步骤, 在该步骤中, 使测井装置选取两个 连续测量点来进行至少两次连续测量;  (a) a homogeneous measurement point selection step in which the logging device selects two consecutive measurement points for at least two consecutive measurements;
( b ) 根据所述两个连续测量点处的测量结果来确定所选取的所 述两个连续测量点是否均能作为均质地层可选点; 如果是, 则  (b) determining, based on the measurements at the two consecutive measurement points, whether the selected two consecutive measurement points are capable of being a homogeneous formation selectable point; if so,
( c ) 根据两个所述均质地层可选点来确定与所测高阻目的层的 地层电阻率相对应的所述测井装置的感应信号的幅度比基值和相位差 基值;  (c) determining, according to the two selected points of the homogeneous formation, an amplitude ratio base value and a phase difference base value of the sensing signal of the logging device corresponding to the formation resistivity of the measured high resistance target layer;
( d ) 根据所述幅度比基值和相位差基值来确定与所测高阻目的 层的地层电阻率相对应的幅度比标准值和相位差标准值;  (d) determining, according to the amplitude ratio base value and the phase difference base value, a magnitude ratio standard value and a phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer;
( e ) 根据所述幅度比标准值和相位差标准值来设定所述所测高 阻目的层的出层阈值;  (e) setting an exit threshold of the measured high resistance target layer according to the amplitude ratio standard value and the phase difference standard value;
( f ) 继续选取下一个测量点进行至少两次测量;  (f) continue to select the next measurement point for at least two measurements;
( g ) 判断在当前测量点处、 测井装置的一对接收线圏之间的感 应电动势的幅度比变化量和 /或相位差变化量是否大于所述出层阈值; (g) determining whether the magnitude ratio change and/or the phase difference variation of the induced electromotive force between the pair of receiving turns of the logging device at the current measurement point is greater than the exit threshold;
( h ) 如果步骤 (g ) 的判断结果为是, 则判定测井装置前方出现 低阻地层。 (h) If the answer in step (g) is YES, then it is determined that a low-resistance formation appears in front of the logging device.
2. 如权利要求 1 所述的测井方法, 其特征在于, 所述步骤 (b ) 进一步包括: 如果任何一个所选取的测量点不能作为均质地层可选点, 则返回步骤 (a ) 以重新选取连续测量点。  2. The logging method according to claim 1, wherein the step (b) further comprises: if any one of the selected measurement points cannot be used as a homogeneous formation selectable point, returning to step (a) Reselect the continuous measurement points.
3. 如权利要求 1 所述的测井方法, 其特征在于, 所述步骤 (b ) 进一步包括:  3. The logging method according to claim 1, wherein the step (b) further comprises:
如果在所选取的测量点之一处、 在所述测井装置的一对接收线圈 之间的感应电动势的幅度比变化量和相位差变化量在其各自的预定阈 值范围内, 则将该测量点作为均质地层可选点。  If the amplitude ratio change amount and the phase difference change amount of the induced electromotive force between one pair of receiving coils of the logging device at one of the selected measuring points are within their respective predetermined threshold values, the measurement is taken Points are optional points for homogeneous formations.
4. 如权利要求 1 所述的测井方法, 其特征在于, 所述步骤 (c ) 进一步包括:  4. The logging method according to claim 1, wherein the step (c) further comprises:
将在所述两个均质地层可选点处所测得的所述一对接收线圏之间 的感应电动势的幅度比的平均值或均方根和相位差的平均值或均方根 分别作为所述幅度比基值和相位差基值。 The mean value or the root mean square and the root mean square of the magnitude of the induced electromotive force between the pair of receiving turns measured at the selectable points of the two homogeneous formations, respectively, or the root mean square As the amplitude ratio base value and phase difference base value.
5. 如权利要求 4所述的测井方法, 其特征在于, 在所述步骤 (c ) 中, 通过磁偶极源并矢格林函数来计算得到所述两个均质地层可选点 处的相应地层电阻率、 幅度比和 /或相位差。 The logging method according to claim 4, wherein in the step (c), the magnetic dipole source dyadic Green's function is used to calculate the selectable points of the two homogeneous formations. Corresponding formation resistivity, amplitude ratio and/or phase difference.
6. 如权利要求 1 所述的测井方法, 其特征在于, 所述步骤 (d ) 进一步包括:  The logging method according to claim 1, wherein the step (d) further comprises:
将所述幅度比基值和相位差基值与预定的各种类型地层的相应本 征值进行比较, 选取与所述幅度比基值和相位差基值最接近的那一种 类型的地层的本征值作为与所测高阻目的层的地层电阻率对应的所述 幅度比标准值和相位差标准值。  Comparing the amplitude to the base value and the phase difference base value to predetermined eigenvalues of the predetermined various types of formations, and selecting the type of the stratum that is closest to the base value and the phase difference base value The eigenvalue is taken as the amplitude ratio standard value and phase difference standard value corresponding to the formation resistivity of the measured high resistance target layer.
7. 如权利要求 1所述的测井方法, 其特征在于, 所述测井方法还 包括:  The logging method according to claim 1, wherein the logging method further comprises:
步骤(i ) , 当步骤(g ) 的判断结果为否时, 存储当前测量点处的 幅度比变化量和相位差变化量, 判断是否到了预定的第 n 个测量点, 如果否, 则返回步骤 (f ) , 其中所述 n为大于 4的自然数。  Step (i), when the judgment result of the step (g) is negative, storing the amplitude ratio change amount and the phase difference change amount at the current measurement point, determining whether the predetermined nth measurement point is reached, and if not, returning to the step (f ) , wherein the n is a natural number greater than 4.
8. 如权利要求 7所述的测井方法, 其特征在于, 所述测井方法还 包括:  The logging method according to claim 7, wherein the logging method further comprises:
步骤(j ),当所述步骤(i )判断当前测量点为所述预定的第 n个测 量点时, 则根据之前存储的各测量点处的幅度比变化量和相位差变化 量来确定幅度比变化趋势和相位差变化趋势。  Step (j), when the step (i) determines that the current measurement point is the predetermined nth measurement point, the amplitude is determined according to the amplitude ratio change amount and the phase difference change amount at each of the previously stored measurement points. The trend of change trend and phase difference.
9. 如权利要求 8所述的测井方法, 其特征在于, 所述测井方法还 包括:  The logging method according to claim 8, wherein the logging method further comprises:
步骤(k ), 如果所述变化趋势为从第 3个测量点到第 n个测量点、 所述幅度比变化量和相位差变化量保持同向递增或总体同向递增, 则 判定所述测井装置的前方出现低阻地层; 否则, 如果既非同向递增也 非总体同向递增, 则判定所述测井装置的前方并未出现低阻地层。  Step (k), if the change trend is from the third measurement point to the nth measurement point, the amplitude ratio change amount and the phase difference change amount keep increasing in the same direction or in the same direction, determining the measurement A low-resistance formation appears in front of the well device; otherwise, if neither the same direction nor the general same direction increases, then it is determined that there is no low-resistance formation in front of the logging device.
10. 一种数据处理设备, 其特征在于, 该数据处理设备包括: 均质地层可选点判定装置 ( 1403、 1404 ) , 其用于判定测井装置 当前所选取的两个连续测量点是否均能作为均质地层可选点;  10. A data processing apparatus, characterized in that the data processing apparatus comprises: a homogeneous layer selectable point determining device (1403, 1404) for determining whether two consecutive measuring points currently selected by the logging device are average Can be used as an optional point for homogeneous formations;
基值确定装置 ( 1406 ) , 其用于在所述均质地层可选点判定装置 ( 1403、 1404 ) 的判断结果为是的情况下, 根据两个所述均质地层可 选点来确定与所测高阻目的层的地层电阻率相对应的所述测井装置的 感应信号的幅度比基值和相位差基值; 标准值确定装置 ( 1407 ) , 其用于根据所述幅度比基值和相位差 基值来确定与所测高阻目的层的地层电阻率对应的幅度比标准值和相 位差标准值; a base value determining device (1406) for determining, based on the two selectable points of the homogeneous formation layer, if the determination result of the homogeneous formation point selectable device (1403, 1404) is YES The amplitude of the induced signal of the logging device corresponding to the formation resistivity of the measured high resistance target layer is greater than the base value and the phase difference base value; a standard value determining device (1407) for determining an amplitude ratio standard value and a phase difference standard value corresponding to a formation resistivity of the measured high resistance target layer according to the amplitude ratio base value and the phase difference base value;
出层阈值设定装置 ( 1408 ) , 其用于根据所述幅度比标准值和相 位差标准值来设定所述所测高阻目的层的出层阈值;  An egress threshold setting device (1408) configured to set an eject threshold of the measured high-resistance target layer according to the amplitude ratio standard value and a phase difference standard value;
第三一第 n 测量点选取及计算装置 ( 1409 ) , 其用于继续选取下 一个测量点进行至少两次测量, 并计算在当前所选取的测量点处、 测 井装置的一对接收线圏之间的感应电动势的幅度比变化量和相位差变 化量; 以及  a third-th nth measuring point selection and calculating device (1409) for continuously selecting the next measuring point for at least two measurements, and calculating a pair of receiving lines of the logging device at the currently selected measuring point The magnitude of the induced electromotive force between the amount of change and the amount of change in phase difference;
低阻地层判定装置( 1410 ) , 其包括出层阈值判定单元( 14101 ) , 该单元用于判断所述当前所选取的测量点处的幅度比变化量和 /或相位 差变化量是否大于所述出层阈值; 如果是, 则判定测井装置前方出现 低阻地层。  a low-resistance formation determining device (1410), comprising an out-of-layer threshold determining unit (14101), configured to determine whether an amplitude ratio change amount and/or a phase difference change amount at the currently selected measurement point is greater than The exit threshold; if so, it is determined that a low-resistance formation is present in front of the logging device.
1 1. 如权利要求 10所述的数据处理设备, 其特征在于, 所述均质 地层可选点判定装置 ( 1403、 1404 ) 用于判断在所选取的测量点处、 在所述测井装置的一对接收线圏之间的感应电动势的幅度比变化量和 相位差变化量是否在其各自的预定阈值范围内, 如果是, 则将参与判 断的所述测量点作为均质地层可选点。  The data processing device according to claim 10, wherein the homogeneous layer selectable point determining means (1403, 1404) is configured to determine at the selected measuring point, in the logging device Whether the magnitude of the induced electromotive force between the pair of receiving coils and the amount of change in the phase difference is within their respective predetermined threshold ranges, and if so, the measuring points participating in the determination are used as the homogeneous layer optional points .
12. 如权利要求 10所述的数据处理设备, 其特征在于, 所述均质 地层可选点判定装置 ( 1403、 1404 ) 如果判断任何一个所选取的测量 点不能作为均质地层可选点, 则指示测井装置重新选取连续测量点。  12. The data processing apparatus according to claim 10, wherein said homogeneous layer selectable point determining means (1403, 1404) determines that any one of the selected measuring points cannot be used as a homogeneous layer selectable point, It then instructs the logging device to reselect the continuous measurement point.
13. 如权利要求 10所述的数据处理设备, 其特征在于, 所述基值 确定装置 ( 1406 ) 进一步被配置为: 将在所述两个均质地层可选点处 所测得的所述一对接收线圏之间的感应电动势的幅度比的平均值或均 方根和相位差的平均值或均方根分别作为所述幅度比基值和相位差基 值。  13. The data processing apparatus according to claim 10, wherein: said base value determining means (1406) is further configured to: said said measured at said select points of said two homogeneous formations The average value or the root mean square or the root mean square of the amplitude ratio of the induced electromotive force between the pair of receiving coil turns as the amplitude ratio base value and the phase difference base value, respectively.
14. 如权利要求 10所述的数据处理设备, 其特征在于, 所述标准 值确定装置 ( 1407 ) 进一步被配置为: 将所述幅度比基值和相位差基 值与预定的各种类型地层的相应本征值进行比较, 选取与所述幅度比 基值和相位差基值最接近的那一种类型的地层的本征值作为与所测高 阻目的层的地层电阻率对应的所述幅度比标准值和相位差标准值。  14. The data processing apparatus according to claim 10, wherein the standard value determining means (1407) is further configured to: base the amplitude ratio base value and the phase difference base value with a predetermined various types of strata Comparing the corresponding eigenvalues, selecting the eigenvalue of the type of the layer closest to the base value and the phase difference base value as the formation corresponding to the formation resistivity of the measured high resistance target layer The amplitude is greater than the standard value and the phase difference standard value.
15. 如权利要求 10所述的数据处理设备, 其特征在于, 所述低阻 地层判定装置 ( 1410) 进一步包括测量点数目判定单元 ( 14102) 和幅 度比及相位差变化趋势判定单元 ( 14103 ) ; 15. The data processing device according to claim 10, wherein said low resistance The formation determining device (1410) further includes a measuring point number determining unit (14102) and an amplitude ratio and phase difference change trend determining unit (14103);
其中所述测量点数目判定单元( 14102)被配置为在所述出层阈值 判定单元 ( 14101 )判断当前测量点的幅度比变化量和相位差变化量不 大于出层阈值时, 判断当前测量点是否已达到预定的第 n个测量点; 如果否, 则指示所述第三-第 n 测量点选取及计算装置 ( 1409) 继续进行下一测量点的选取及幅度比变化量和相位差变化量的计算; 反之, 如果当前测量点为预定的第 n 个测量点, 则指示幅度比及 相位差变化趋势确定单元 ( 14103 ) 来根据之前所存储的各测量点处的 幅度比变化量和相位差变化量来确定幅度比变化趋势和相位差变化趋 势。  The measurement point number determining unit (14102) is configured to determine the current measurement point when the exit layer threshold determining unit (14101) determines that the amplitude ratio change amount and the phase difference change amount of the current measurement point are not greater than the exit layer threshold value. Whether the predetermined nth measurement point has been reached; if not, instructing the third-nth measurement point selection and calculation device (1409) to continue the selection of the next measurement point and the amplitude ratio change amount and the phase difference change amount On the other hand, if the current measurement point is the predetermined nth measurement point, the amplitude ratio and phase difference change trend determining unit (14103) is indicated to vary the amplitude ratio and the phase difference according to the previously stored measurement points. The amount of change is used to determine the trend of the amplitude ratio change trend and the phase difference.
16. 如权利要求 15所述的数据处理设备, 其特征在于, 所述低阻 地层判定装置( 1410)进一步包括同向递增变化趋势判定单元( 14104), 所述同向递增变化趋势判定单元( 14104) 用于判断由所述幅度比及相 位差变化趋势确定单元( 14103 )确定的所述变化趋势是否为从第三个 测量点到第 n 个测量点, 所述幅度比变化量和相位差变化量保持同向 递增, 如果是, 则判定所述测井装置的前方为低阻地层。  The data processing device according to claim 15, wherein the low-resistance formation determining means (1410) further comprises a co-directional incremental change trend determining unit (14104), and the co-directional incremental change trend determining unit ( 14104) configured to determine whether the change trend determined by the amplitude ratio and phase difference change trend determining unit (14103) is from a third measurement point to an nth measurement point, the amplitude ratio change amount and phase difference The amount of change remains increasing in the same direction, and if so, it is determined that the front of the logging device is a low resistance formation.
17. 如权利要求 16所述的数据处理设备, 其特征在于, 所述低阻 地层判定装置 ( 1410 ) 进一步包括总体同向递增变化趋势判定单元 17. The data processing apparatus according to claim 16, wherein the low resistance formation determining means (1410) further comprises an overall co-directional incremental change trend determining unit
( 14105 ) , 其用于在判定单元 ( 14104) 的判定结果为否时判断所述 变化趋势是否总体为同向递增, 如果是, 则判定为所述测井装置的前 方为低阻地层; 如果否, 则判定所述测井装置的前方没有出现低阻地 层。 (14105), configured to determine whether the change trend is generally in the same direction when the determination result of the determining unit (14104) is negative, and if yes, determine that the front of the logging device is a low-resistance formation; Otherwise, it is determined that there is no low resistance formation in front of the logging device.
18. —种测井装置,其特征在于, 所述测井装置包括钻铤本体( 12) 和天线阵列, 其中所述天线阵列包括至少一对发射天线和接收天线, 所述发射天线和接收天线用于生成前向探测深度曲线。  18. A logging device, characterized in that the logging device comprises a drill collar body (12) and an antenna array, wherein the antenna array comprises at least one pair of transmitting antennas and receiving antennas, the transmitting antenna and the receiving antenna Used to generate a forward probing depth curve.
19. 如权利要求 18所述的测井装置, 其特征在于, 所述天线阵列 包括 4个发射天线 T1 ( 11 ) 、 T2 ( 14) 、 T3 ( 13 ) 和 T4 ( 15 ) , 以 及 4个接收天线 R1 ( 7 ) 、 R2 ( 8 ) 、 R3 ( 9 ) 和 R4 ( 10 ) 。  19. The logging device according to claim 18, wherein the antenna array comprises four transmitting antennas T1 (11), T2 (14), T3 (13) and T4 (15), and four receiving Antennas R1 ( 7 ) , R2 ( 8 ) , R3 ( 9 ) and R4 ( 10 ).
20. 如权利要求 19所述的测井装置, 其特征在于, 所述天线阵列 从所述钻挺本体 ( 12 ) 的钻挺尾端到钻头端的排列顺序为: 接收天线 R3、 发射天线 T3、 发射天线 Tl、 接收天线 Rl、 接收天线 R2、 发射天 线 T2、 发射天线 Τ4、 和接收天线 R4; 所述接收天线 R1和 R2之间的 中点为测量点, 所述发射天线 T1 与 Τ2、 Τ3 与 Τ4分别以该测量点为 中心对称地安装;所述接收天线 R 1和 R2的安装角度均基本上为零度; 所述接收天线 R3和 R4以所述测量点为对称中心设置在所述钻铤本体 ( 12 ) 的两端, 并且所述接收天线 R3和 R4的安装角分别被设置为约 45° 和约 -45° 。 The logging device according to claim 19, wherein the antenna array is arranged from the tail end of the drill collar body (12) to the drill bit end: a receiving antenna R3, a transmitting antenna T3, Transmitting antenna Tl, receiving antenna Rl, receiving antenna R2, transmitting day a line T2, a transmitting antenna Τ4, and a receiving antenna R4; a midpoint between the receiving antennas R1 and R2 is a measuring point, and the transmitting antennas T1 and Τ2, Τ3 and Τ4 are respectively symmetrically mounted with the measuring point as a center; The mounting angles of the receiving antennas R 1 and R2 are substantially zero degrees; the receiving antennas R3 and R4 are disposed at both ends of the drill collar body ( 12 ) with the measuring points as a center of symmetry, and the receiving The mounting angles of the antennas R3 and R4 are set to about 45° and about -45°, respectively.
PCT/CN2011/002099 2010-12-23 2011-12-14 Well logging device, well logging method and data processing apparatus WO2012083585A1 (en)

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NO20131015A NO346394B1 (en) 2010-12-23 2011-12-14 A device and method for well logging and data processing device
CA2822506A CA2822506C (en) 2010-12-23 2011-12-14 A device and method for determining the resistivity of a formation in front of a well logger
JP2013545012A JP5944923B2 (en) 2010-12-23 2011-12-14 Physical logging equipment, physical logging method, and data processing apparatus
US15/167,490 US9927548B2 (en) 2010-12-23 2016-05-27 Apparatus for well logging capable of forward investigation

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